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<front>
<journal-meta>
<journal-id journal-id-type="publisher-id">Front. Physiol.</journal-id>
<journal-title>Frontiers in Physiology</journal-title>
<abbrev-journal-title abbrev-type="pubmed">Front. Physiol.</abbrev-journal-title>
<issn pub-type="epub">1664-042X</issn>
<publisher>
<publisher-name>Frontiers Media S.A.</publisher-name>
</publisher>
</journal-meta>
<article-meta>
<article-id pub-id-type="doi">10.3389/fphys.2018.00273</article-id>
<article-categories>
<subj-group subj-group-type="heading">
<subject>Physiology</subject>
<subj-group>
<subject>Original Research</subject>
</subj-group>
</subj-group>
</article-categories>
<title-group>
<article-title>Center of Pressure Motion After Calf Vibration Is More Random in Fallers Than Non-fallers: Prospective Study of Older Individuals</article-title>
</title-group>
<contrib-group>
<contrib contrib-type="author" corresp="yes">
<name><surname>van den Hoorn</surname> <given-names>Wolbert</given-names></name>
<xref ref-type="aff" rid="aff1"><sup>1</sup></xref>
<xref ref-type="author-notes" rid="fn001"><sup>&#x0002A;</sup></xref>
<uri xlink:href="http://loop.frontiersin.org/people/169022/overview"/>
</contrib>
<contrib contrib-type="author">
<name><surname>Kerr</surname> <given-names>Graham K.</given-names></name>
<xref ref-type="aff" rid="aff2"><sup>2</sup></xref>
<uri xlink:href="http://loop.frontiersin.org/people/65022/overview"/>
</contrib>
<contrib contrib-type="author">
<name><surname>van Die&#x000EB;n</surname> <given-names>Jaap H.</given-names></name>
<xref ref-type="aff" rid="aff3"><sup>3</sup></xref>
<uri xlink:href="http://loop.frontiersin.org/people/129838/overview"/>
</contrib>
<contrib contrib-type="author">
<name><surname>Hodges</surname> <given-names>Paul W.</given-names></name>
<xref ref-type="aff" rid="aff1"><sup>1</sup></xref>
</contrib>
</contrib-group>
<aff id="aff1"><sup>1</sup><institution>Centre for Clinical Research Excellence in Spinal Pain, Injury and Health, School of Health &#x00026; Rehabilitation Sciences, The University of Queensland</institution>, <addr-line>Brisbane, QLD</addr-line>, <country>Australia</country></aff>
<aff id="aff2"><sup>2</sup><institution>Movement Neuroscience Program, Institute of Health and Biomechanical Innovation, Queensland University of Technology</institution>, <addr-line>Brisbane, QLD</addr-line>, <country>Australia</country></aff>
<aff id="aff3"><sup>3</sup><institution>Amsterdam Movement Sciences, Department of Human Movement Sciences, Vrije Universiteit Amsterdam</institution>, <addr-line>Amsterdam</addr-line>, <country>Netherlands</country></aff>
<author-notes>
<fn fn-type="edited-by"><p>Edited by: Plamen Ch. Ivanov, Boston University, United States</p></fn>
<fn fn-type="edited-by"><p>Reviewed by: Valerie Livina, National Physical Laboratory, United Kingdom; Chengyu Huo, Changshu Institute of Technology, China</p></fn>
<fn fn-type="corresp" id="fn001"><p>&#x0002A;Correspondence: Wolbert van den Hoorn <email>w.vandenhoorn&#x00040;uq.edu.au</email></p></fn>
<fn fn-type="other" id="fn002"><p>This article was submitted to Fractal Physiology, a section of the journal Frontiers in Physiology</p></fn></author-notes>
<pub-date pub-type="epub">
<day>26</day>
<month>03</month>
<year>2018</year>
</pub-date>
<pub-date pub-type="collection">
<year>2018</year>
</pub-date>
<volume>9</volume>
<elocation-id>273</elocation-id>
<history>
<date date-type="received">
<day>07</day>
<month>12</month>
<year>2017</year>
</date>
<date date-type="accepted">
<day>08</day>
<month>03</month>
<year>2018</year>
</date>
</history>
<permissions>
<copyright-statement>Copyright &#x000A9; 2018 van den Hoorn, Kerr, van Die&#x000EB;n and Hodges.</copyright-statement>
<copyright-year>2018</copyright-year>
<copyright-holder>van den Hoorn, Kerr, van Die&#x000EB;n and Hodges</copyright-holder>
<license xlink:href="http://creativecommons.org/licenses/by/4.0/"><p>This is an open-access article distributed under the terms of the Creative Commons Attribution License (CC BY). The use, distribution or reproduction in other forums is permitted, provided the original author(s) and the copyright owner are credited and that the original publication in this journal is cited, in accordance with accepted academic practice. No use, distribution or reproduction is permitted which does not comply with these terms.</p></license>
</permissions>
<abstract><p>Aging is associated with changes in balance control and elderly take longer to adapt to changing sensory conditions, which may increase falls risk. Low amplitude calf muscle vibration stimulates local sensory afferents/receptors and affects sense of upright when applied in stance. It has been used to assess the extent the nervous system relies on calf muscle somatosensory information and to rapidly change/perturb part of the somatosensory information causing balance unsteadiness by addition and removal of the vibratory stimulus. This study assessed the effect of addition and removal of calf vibration on balance control (in the absence of vision) in elderly individuals (&#x0003E;65 years, <italic>n</italic> &#x0003D; 99) who did (<italic>n</italic> &#x0003D; 41) or did not prospectively report falls (<italic>n</italic> &#x0003D; 58), and in a group of young individuals (18&#x02013;25 years, <italic>n</italic> &#x0003D; 23). Participants stood barefoot and blindfolded on a force plate for 135 s. Vibrators (60 Hz, 1 mm) attached bilaterally over the triceps surae muscles were activated twice for 15 s; after 15 and 75 s (45 s for recovery). Balance measures were applied in a windowed (15 s epoch) manner to compare center-of-pressure (CoP) motion before, during and after removal of calf vibration between groups. In each epoch, CoP motion was quantified using linear measures, and non-linear measures to assess temporal structure of CoP motion [using recurrence quantification analysis (RQA) and detrended fluctuation analysis]. Mean CoP displacement during and after vibration did not differ between groups, which suggests that calf proprioception and/or weighting assigned by the nervous system to calf proprioception was similar for the young and both groups of older individuals. Overall, compared to the elderly, CoP motion of young was more predictable and persistent. Balance measures were not different between fallers and non-fallers before and during vibration. However, non-linear aspects of CoP motion of fallers and non-fallers differed after removal of vibration, when dynamic re-weighting is required. During this period fallers exhibited more random CoP motion, which could result from a reduced ability to control balance and/or a reduced ability to dynamically reweight proprioceptive information. These results show that non-linear measures of balance provide evidence for deficits in balance control in people who go on to fall in the following 12 months.</p></abstract>
<kwd-group>
<kwd>aging</kwd>
<kwd>muscle vibration</kwd>
<kwd>balance</kwd>
<kwd>somatosensory</kwd>
<kwd>proprioception</kwd>
<kwd>falls</kwd>
<kwd>recurrence quantification analysis</kwd>
<kwd>detrended fluctuation analysis</kwd>
</kwd-group>
<contract-num rid="cn001">ID443210</contract-num>
<contract-num rid="cn001">APP1091302</contract-num>
<contract-num rid="cn001">APP1102905</contract-num>
<contract-sponsor id="cn001">National Health and Medical Research Council<named-content content-type="fundref-id">10.13039/501100000925</named-content></contract-sponsor>
<counts>
<fig-count count="6"/>
<table-count count="4"/>
<equation-count count="0"/>
<ref-count count="98"/>
<page-count count="17"/>
<word-count count="12391"/>
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</article-meta>
</front>
<body>
<sec sec-type="intro" id="s1">
<title>Introduction</title>
<p>Falls and falls related injuries are a serious health issue (Hill et al., <xref ref-type="bibr" rid="B44">2004</xref>) in the aging population and poor balance control is a major contributor (Campbell et al., <xref ref-type="bibr" rid="B13">1989</xref>; Maki et al., <xref ref-type="bibr" rid="B55">1994</xref>). Balance control requires sense of the body&#x00027;s vertical with respect to gravity and sense of deviations away from the vertical with the goal to maintain the body&#x00027;s center of mass within the base of support (Horak, <xref ref-type="bibr" rid="B45">2006</xref>). In addition to overall perception of orientation with respect to gravity, mostly provided by the vestibular system (Day and Fitzpatrick, <xref ref-type="bibr" rid="B18">2005</xref>), feedback of the relative positions and movements of body segments is provided by somatosensation, and global orientation and movement is provided by vision (Proske and Gandevia, <xref ref-type="bibr" rid="B71">2012</xref>). Sensory information is dynamically processed by the central nervous system (CNS), and appropriate corrections are applied by the motor system. Physiological aging is associated with diminished functioning of these systems and underpins some of the decline in balance control (Lord et al., <xref ref-type="bibr" rid="B52">1991</xref>). Why some older individuals fall whereas others do not might plausibly be explained by variation in the decline of the somatosensory input and the impact of somatosensory changes on balance control.</p>
<p>Somatosensory information from muscle spindles in postural muscles is important for standing balance control (Horak, <xref ref-type="bibr" rid="B45">2006</xref>; Proske and Gandevia, <xref ref-type="bibr" rid="B71">2012</xref>). Somatosensory function can be assessed with low amplitude vibration of the muscle-tendon complex, which increases the discharge rate of muscle spindle Ia afferents (Burke et al., <xref ref-type="bibr" rid="B12">1976</xref>; Roll et al., <xref ref-type="bibr" rid="B79">1989</xref>) in a 1:1 relation with the vibratory stimulus (Roll et al., <xref ref-type="bibr" rid="B79">1989</xref>), and creates an illusion of muscle lengthening (Goodwin et al., <xref ref-type="bibr" rid="B35">1972</xref>). If the vibrated muscle serves a postural function, the illusory change in muscle length induces an illusory change in the sense of upright, and posture is automatically adjusted (Eklund, <xref ref-type="bibr" rid="B31">1972</xref>; Barbieri et al., <xref ref-type="bibr" rid="B6">2008</xref>). The magnitude of corrective center-of-pressure (CoP) displacement (i.e., reflection of the postural adaptation) reflects both the <italic>sensitivity</italic> of muscle spindles to vibration and the <italic>relative weighting</italic> that the CNS places on the contribution of the spindle input to the perception and control of posture (Brumagne et al., <xref ref-type="bibr" rid="B10">2004</xref>).</p>
<p>The CoP response to triceps surae (calf) vibration in standing is affected by age, but findings are inconsistent. Postural responses of older individuals have been reported to be less (Pyykk&#x000F6; et al., <xref ref-type="bibr" rid="B72">1990</xref>; Quoniam et al., <xref ref-type="bibr" rid="B73">1995</xref>; Hay et al., <xref ref-type="bibr" rid="B43">1996</xref>), more (Maitre et al., <xref ref-type="bibr" rid="B54">2013</xref>), or similar (Brumagne et al., <xref ref-type="bibr" rid="B10">2004</xref>; Abrahamov&#x000E1; et al., <xref ref-type="bibr" rid="B2">2009</xref>) to those in young individuals. Although, this variation in outcomes can partly be explained by differences in participant ages (Brumagne et al., <xref ref-type="bibr" rid="B10">2004</xref>), differences in postural perturbation paradigms and small sample sizes, variable findings could also suggest that age-related changes in somatosensory functioning vary between individuals, placing some individuals at higher risk for falling.</p>
<p>Changes in the environment in daily life (e.g., lighting and support surface conditions) require constant re-weighting of somatosensory information to aid balance control. Aging affects the ability to flexibly reconfigure proprioception for postural control to changes in proprioceptive context (Hay et al., <xref ref-type="bibr" rid="B43">1996</xref>; Sturnieks et al., <xref ref-type="bibr" rid="B88">2008</xref>; Eikema et al., <xref ref-type="bibr" rid="B29">2013</xref>, <xref ref-type="bibr" rid="B30">2014</xref>). Sense of upright and balance control are perturbed by both addition and removal of the muscle vibration stimulus. Addition of vibration distorts part of, and contradicts, the total afferent source, causing balance unsteadiness (Eklund, <xref ref-type="bibr" rid="B31">1972</xref>). Removal of vibration can cause the illusory change in upright posture to reverse (Wierzbicka et al., <xref ref-type="bibr" rid="B97">1998</xref>; Duclos et al., <xref ref-type="bibr" rid="B27">2007</xref>) again inducing balance unsteadiness. Balance unsteadiness after vibration removal is likely to be mediated, at least in part, by a transient reduction of discharge/sensitivity of muscle spindles (Rogers et al., <xref ref-type="bibr" rid="B78">1985</xref>), and by time required by the CNS to dynamically re-weight available sensory systems (Brumagne et al., <xref ref-type="bibr" rid="B10">2004</xref>; van der Kooij and Peterka, <xref ref-type="bibr" rid="B93">2011</xref>). The ability to flexibly explore somatosensory redundancy (i.e., <italic>re-weighting</italic>) could be beneficial for balance control to minimize the perturbation effects on balance caused by addition and removal of muscle vibration. If not, this might result in increased unsteadiness during and after removal of the vibratory stimulus which could be linked with falls risk.</p>
<p>Linear measures of balance parameters such as sway path length or root mean square (RMS) velocity implicitly assume that the temporal structure of CoP motion arises from random fluctuations in the postural control system that do not change over time. These measures have been used in most investigations of the effect of muscle vibration on postural control. Although linear measures are affected by vibration, they offer little insight into the dynamic characteristics of CoP motion in response to vibration perturbations, which is likely to aid interpretation of the underlying mechanisms. Non-linear measures such as recurrence quantification analysis (RQA) (Eckmann et al., <xref ref-type="bibr" rid="B28">1987</xref>; Marwan et al., <xref ref-type="bibr" rid="B59">2007</xref>) and detrended fluctuation analysis (DFA) (Peng et al., <xref ref-type="bibr" rid="B69">1995b</xref>) describe the temporal structure of CoP motion. The adaptable multisensory integration and response generation of optimal balance control (Nashner, <xref ref-type="bibr" rid="B63">1976</xref>) results in balance performance that is resilient to small perturbations; quantified using RQA as a measure of the structure of recurrent CoP motion (Riley et al., <xref ref-type="bibr" rid="B75">1999</xref>; Marwan et al., <xref ref-type="bibr" rid="B59">2007</xref>), appears smooth and persistent; which is measured with DFA (Peng et al., <xref ref-type="bibr" rid="B69">1995b</xref>). Measures obtained with these non-linear methods change when postural control is challenged (Riley et al., <xref ref-type="bibr" rid="B75">1999</xref>; Riley and Clark, <xref ref-type="bibr" rid="B77">2003</xref>), and can distinguish elderly from young individuals (Norris et al., <xref ref-type="bibr" rid="B66">2005</xref>; Amoud et al., <xref ref-type="bibr" rid="B3">2007</xref>; Duarte and Sternad, <xref ref-type="bibr" rid="B26">2008</xref>; Kim et al., <xref ref-type="bibr" rid="B50">2008</xref>; Seigle et al., <xref ref-type="bibr" rid="B83">2009</xref>), although findings vary, (Seigle et al., <xref ref-type="bibr" rid="B83">2009</xref>; Wang and Yang, <xref ref-type="bibr" rid="B95">2012</xref>). These non-linear measures are likely to provide a more detailed understanding of how sensory perturbations impact balance control.</p>
<p>This study aimed to: (i) compare CoP motion between young and older individuals before, during and after removal of bilateral calf vibration, and (ii) compare measures between older individual who subsequently do or do not go on to fall in the following 12 months. We probed this question using linear and non-linear measures of CoP motion to investigate impact of addition and removal of vibration to the calf muscles.</p>
</sec>
<sec sec-type="methods" id="s2">
<title>Methods</title>
<sec>
<title>Participants</title>
<p>One-hundred-and-six participants older than 65 years of age volunteered for this study (42 female, 64 male) with a mean &#x000B1; <italic>SD</italic> age, weight and height of 75 &#x000B1; 6 years, 78 &#x000B1; 15 kg, 1.69 &#x000B1; 0.09 m, respectively. Participants were a subset from a larger cohort (<italic>n</italic> &#x0003D; 252), and were included in the current study based on the Physiological Profile Assessment score (PPA, short form version) of Lord et al. (<xref ref-type="bibr" rid="B53">2003</xref>). To ensure a wide range of falls risk, participants were included in the current study if their PPA values were below 0.5 (<italic>n</italic> &#x0003D; 59) or above 1 (<italic>n</italic> &#x0003D; 47). All participants were recruited from the Brisbane metropolitan area via the Australian electoral role. A letter of invitation was sent with an information sheet, which outlined the potential risks and benefits of the research. Participants were excluded if they had a recent or recurrent history of surgery or musculoskeletal injury, any neurological impairment such as Parkinson&#x00027;s disease, were unable to ambulate independently without the use of a walking aid, or were cognitively impaired (i.e., Mini mental state exam score &#x0003C;24). The young group included 23 participants between 18 and 25 years of age (14 female, 9 male, 21 &#x000B1; 2 years, 65 &#x000B1; 10 kg, 1.72 &#x000B1; 0.05 m) recruited from the student population of local universities and by word of mouth. All participants provided written informed consent. The experimental protocol was approved by the Institutional Human Research Ethics Committees and conformed to the Declaration of Helsinki.</p>
</sec>
<sec>
<title>Prospective falls measurement</title>
<p>Elderly participants were followed for 12 months after the balance assessment. They maintained a weekly falls diary, which they returned at the end of each month via reply paid post (Hannan et al., <xref ref-type="bibr" rid="B39">2010</xref>). A fall was defined as: &#x0201C;an unintentionally coming to the ground or some other lower level, not as a result of a major intrinsic event (e.g., stroke) or overwhelming hazard. This included any slips, trips or accidents, which result in a fall onto a lower level, be it a chair, bed or the floor for example.&#x0201D; A &#x0201C;faller&#x0201D; was defined as a person who had one or more falls recorded within the 12-month follow-up period.</p>
</sec>
<sec>
<title>Experimental setup and procedure</title>
<p>Participants stood barefoot on a force plate (Type 9286AA, Kistler Group, Winterthur, Switzerland), were blindfolded to exclude the contribution of vision to balance, and wore headphones playing white noise to limit distraction. Participants stood relaxed with arms hanging by their sides and data collection commenced after &#x0007E;20 s to ensure balance had reached a steady state.</p>
<p>Participants stood for 135 s after commencement of data recording. Custom-made vibrators (Type YM2707, Electus Distribution, Sydney, Australia, &#x0007E;1 mm, 60 Hz) were bilaterally attached halfway between the distal portion of the gastrocnemius muscle heads and the distal insertion of the Achilles tendon. Firm application was assured with pressure applied to the vibrators using a neoprene band wrapped around the ankle and vibrator. After 15 s, mechanical vibration was applied bilaterally for 15 s. Vibrators were switched on for a further 15 s period at 75 s from commencement of recording. This allowed 45 s after cessation of each vibration exposure to assess post-vibration effects on balance. The experimenter stood close to the participant to provide support in case of falling. If balance was assisted, data collection was stopped and restarted if the participant agreed.</p>
<p>Force plate data were amplified [Type 5233A, (range: Fx &#x00026; Fy; 250N, Fz; 2500N), Kistler Group, Winterthur, Switzerland] and digitized with 16-bit precision at a sampling rate of 2,000 samples/s using a Power 1401 data acquisition system with Spike2 software (Cambridge Electronic Design Limited, Cambridge, UK).</p>
</sec>
<sec>
<title>Data analysis</title>
<p>Data were analyzed offline with Matlab (Mathworks inc., Natick, MA, USA). As calf vibration mainly perturbs balance in the anterior-posterior direction (Eklund, <xref ref-type="bibr" rid="B31">1972</xref>), analyses were focused on CoP motion in this plane. CoP data were filtered using a second order low pass bi-directional Butterworth filter. Cut-off frequency was set at 20 Hz and bi-directional filtering increased the filter order to 4. After low-pass filtering, data were decimated to 100 samples/s. All measures were applied in a windowed (15-s epoch) manner (Riley et al., <xref ref-type="bibr" rid="B75">1999</xref>; Webber and Marwan, <xref ref-type="bibr" rid="B96">2014</xref>), to assess changes in CoP motion during and after calf vibration (see Figure <xref ref-type="fig" rid="F1">1</xref> for details).</p>
<fig id="F1" position="float">
<label>Figure 1</label>
<caption><p>Recurrence quantification analysis methods. <bold>(A)</bold> CoP motion in anterior-posterior example of a participant (faller) showing baseline, first and second vibrations (VIB) and 45 s after each vibration. Data were analyzed using 15-s epochs (ep). This includes the vibration epoch, and epochs 1&#x02013;31 (post vibration epochs), which started after cessation of vibration and was shifted in time with 1-s intervals (93.33% overlap) until 45 s after vibration to assess balance after vibration. This resulted in two sets (two vibration repetitions) of 32 epochs (1 vibration &#x0002B; 31 post vibration) for each participant which were used for statistical analysis to assess group differences. Group differences at the baseline epoch were assessed separately as there was only 1 repetition available (see Statistics section for more details). <bold>(B)</bold> Example of a CoP epoch (blue) delayed with a tau of 180 ms. <bold>(C)</bold> A phase space was created by plotting the delayed CoP copies against each other. Note that the example is given in 3D, but, analysis was performed in 5D. <bold>(D)</bold> The recurrence plot represents the recurrences of CoP in the phase space depicted in <bold>(C)</bold>; by creating a 2D recurrence plot by adapting the recurrence threshold distance to fix the recurrence rate to 5%. Temporally close recurrences were excluded (&#x0003C;1 s, Theiler window) which is represented by the grayed area along the line of identity (were CoP recurs with itself). Two examples are shown that represent a diagonal (in light and dark green) and vertical recurrence structures (in red). These examples are also shown in the phase space in <bold>(C)</bold>. The light and dark green represents CoP motion running parallel in phase space and the red line represents CoP motion that revisits and remains in a region in phase space represented by the red dot in <bold>(C)</bold> and <bold>(D)</bold>.</p></caption>
<graphic xlink:href="fphys-09-00273-g0001.tif"/>
</fig>
<sec>
<title>Description of CoP motion</title>
<p>The CoP is the baricenter of the contact surface of an individual on the ground, or in other words the point of application of the ground reaction force. CoP motion provides a proxy measure of standing balance dynamics. CoP motion contains information regarding the motion of the vertical projection of the center of mass of the whole body and of the moments that are generated by the individual (Winter, <xref ref-type="bibr" rid="B98">1995</xref>). For example, forward body lean involves a forward position of the center of mass, which is reflected in a forward position of the CoP. Moving the center of mass backwards by rotation around the ankle joints requires generation of ankle moments which shift the CoP further anterior relative to the center of mass.</p>
</sec>
<sec>
<title>Linear measures</title>
<p>Sway path (SP, mms<sup>&#x02212;1</sup>) was calculated as the sum of the absolute distances between consecutive data points divided by epoch length. CoP position (mm), relative to the mean CoP position at the baseline pre-vibration epoch, was calculated as the mean position of CoP within each epoch.</p>
</sec>
<sec>
<title>Non-linear measures</title>
<sec>
<title>Recurrence quantification analysis</title>
<p>CoP dynamics were captured by plotting time delayed copies of the CoP signal against each other [methods of delay (Takens, <xref ref-type="bibr" rid="B90">1981</xref>), see Figure <xref ref-type="fig" rid="F1">1C</xref> for a 3-dimensional representation]. The phase space dimension was fixed at 5 dimensions determined with false nearest neighbor analysis (Kennel et al., <xref ref-type="bibr" rid="B49">1992</xref>) using the whole signal (135 s). The delay was calculated using the average displacement method (Rosenstein et al., <xref ref-type="bibr" rid="B81">1994</xref>) also using the whole signal, for each participant individually. Phase space dimension was limited to 5 dimensions as higher dimensional phase space would require longer time series (Grassberger and Procaccia, <xref ref-type="bibr" rid="B36">1983</xref>; Marwan, <xref ref-type="bibr" rid="B58">2011</xref>) and true recurrences might be missed (Marwan, <xref ref-type="bibr" rid="B58">2011</xref>). The points in this volume (or phase space), represent the history of all balance solutions (or states). Recurrences of balance solutions within this phase space were visualized by a 2-dimensional recurrence plot (Eckmann et al., <xref ref-type="bibr" rid="B28">1987</xref>), which represents the times at which balance solutions revisit (recur) in phase space (Webber and Marwan, <xref ref-type="bibr" rid="B96">2014</xref>). RQA describes the features of these recurrences. Figure <xref ref-type="fig" rid="F1">1</xref> shows the details of the RQA method and settings used. Table <xref ref-type="table" rid="T1">1</xref> provides definitions and interpretations of RQA parameters in relation to CoP motion.</p>
<table-wrap position="float" id="T1">
<label>Table 1</label>
<caption><p>Definition and interpretation of recurrence quantification analysis (RQA) and detrended fluctuation analysis (DFA) in the context of the balance task.</p></caption>
<table frame="hsides" rules="groups">
<thead><tr>
<th/>
<th valign="top" align="left"><bold>Variable</bold></th>
<th valign="top" align="left"><bold>Definition</bold></th>
<th valign="top" align="left"><bold>Higher value interpretation</bold></th>
<th valign="top" align="left"><bold>Lower value interpretation</bold></th>
</tr>
</thead>
<tbody>
<tr>
<td valign="top" align="left">RQA diagonal</td>
<td valign="top" align="left">%DET</td>
<td valign="top" align="left">The percentage of all recurrences in phase space (below a pre-set threshold distance) that form diagonal line lengths longer than 100 ms</td>
<td valign="top" align="left">More predictable, more deterministic, less random CoP motion, consistent with better balance performance</td>
<td valign="top" align="left">Less predictable, less deterministic, more random CoP motion, consistent with reduced balance performance</td>
</tr>
<tr style="border-bottom: thin solid #000000;">
<td/>
<td valign="top" align="left">L<sub>mean</sub></td>
<td valign="top" align="left">The mean length of the diagonal lines in the recurrence plot</td>
<td valign="top" align="left">Better balance performance, less impact of small perturbations resulting in more similar temporal dynamic CoP patterns</td>
<td valign="top" align="left">Reduced balance performance, greater impact of small perturbations, resulting in less similar (more random) temporal dynamic CoP patterns</td>
</tr> <tr>
<td valign="top" align="left">RQA vertical</td>
<td valign="top" align="left">%LAM</td>
<td valign="top" align="left">The percentage of all recurrences in phase space (below a pre-set threshold distance) that form vertical line lengths longer than 100 ms</td>
<td valign="top" align="left">More intermittent CoP motion with more periods of minimal CoP fluctuations</td>
<td valign="top" align="left">Less intermittent CoP motion with fewer periods of minimal CoP fluctuations</td>
</tr>
<tr style="border-bottom: thin solid #000000;">
<td/>
<td valign="top" align="left">TT</td>
<td valign="top" align="left">The mean length of the vertical lines in the recurrence plot</td>
<td valign="top" align="left">Longer periods of minimal CoP fluctuations (static states)</td>
<td valign="top" align="left">Shorter periods of minimal CoP fluctuations (static states)</td>
</tr> <tr>
<td valign="top" align="left">DFA</td>
<td valign="top" align="left">DFA<sub>1</sub></td>
<td valign="top" align="left">Exponential interrelation of CoP fluctuations at time scales between 0.1 and tau s</td>
<td valign="top" align="left">Smoother and more persistent CoP motion at time scales &#x0003C; tau</td>
<td valign="top" align="left">Less smooth and less persistent CoP movements at time scales &#x0003C; tau</td>
</tr>
<tr>
<td/>
<td valign="top" align="left">DFA<sub>2</sub></td>
<td valign="top" align="left">Exponential interrelation of CoP fluctuations at time scales between tau and 4.42 s</td>
<td valign="top" align="left">Smoother and less anti persistent CoP motion at time scales &#x0003E; tau</td>
<td valign="top" align="left">Less smooth and more anti persistent CoP motion at time scales &#x0003E; tau</td>
</tr>
<tr>
<td/>
<td valign="top" align="left">DFA<sub>tau</sub></td>
<td valign="top" align="left">The time scale that separates DFA short and DFA long</td>
<td valign="top" align="left">Less conservative balance control</td>
<td valign="top" align="left">More conservative balance control</td>
</tr>
</tbody>
</table>
<table-wrap-foot>
<p><italic>Recurrence quantification analysis (RQA), diagonal line structures; percentage determinism (%DET), mean diagonal line length (L<sub>mean</sub>), vertical line structure; percentage laminarity (%LAM), mean vertical line length (trapping time, TT). Detrended fluctuation analysis (DFA), short term DFA (DFA<sub>1</sub>), longer term DFA (DFA<sub>2</sub>) and the time scale that separates DFA<sub>1</sub> and DFA<sub>2</sub>; DFA<sub>tau.</sub></italic></p>
</table-wrap-foot>
</table-wrap>
<p>The features of the recurrence plot using RQA were quantified by the diagonal lines; the percentage determinism (%DET), mean diagonal line lengths (L<sub>mean</sub>), and vertical lines; the percentage laminarity (%LAM) and trapping time (TT) using Marwan&#x00027;s RQA toolbox (Marwan, <xref ref-type="bibr" rid="B57">1998</xref>; Marwan et al., <xref ref-type="bibr" rid="B59">2007</xref>). To avoid ceiling effect of the %DET and %LAM, sensitivity was reduced by considering 0.1 s as a minimal length of both diagonal and vertical line features (Seigle et al., <xref ref-type="bibr" rid="B83">2009</xref>; Ramdani et al., <xref ref-type="bibr" rid="B74">2013</xref>).</p>
<p>The level of recurrence rate impacts the recurrence quantification (Riley et al., <xref ref-type="bibr" rid="B75">1999</xref>). Therefore, the recurrence threshold, below which a recurrence was defined, is usually dependent on some measure of CoP motion amplitude, such as percentage of the maximum diameter of balance states within the phase space (Ramdani et al., <xref ref-type="bibr" rid="B74">2013</xref>; Decker et al., <xref ref-type="bibr" rid="B19">2015</xref>) or percentage of mean distance between al data points in phase space (Riley et al., <xref ref-type="bibr" rid="B75">1999</xref>; Riley and Clark, <xref ref-type="bibr" rid="B77">2003</xref>). However, because the size of the diameter of balance states is biased by larger CoP motion excursion and because not all areas in phase space will be revisited equally frequently, the amplitude measures that are used to set the recurrence threshold could skew the resulting recurrence rate, and therefore the recurrence quantification. This would be more likely to be problematic in shorter time series. Therefore, we adapted the recurrence threshold to fix the recurrence rate to 5% to avoid these issues and to have a more scale free RQA and to enable better comparison between groups at each CoP window.</p>
<p><italic>Diagonal line features</italic>. Diagonal line features extracted from the recurrence plot, reflect the deterministic behavior of CoP motion, respectively (Figures <xref ref-type="fig" rid="F1">1C,D</xref>). The percentage of recurrences that form diagonal lines (%DET) and the mean diagonal line length (L<sub>mean</sub>) are positively linked with the predictability, i.e., the deterministic pattern of CoP motion, as similar balance solutions (states) will lead to similar CoP temporal patterns (Webber and Marwan, <xref ref-type="bibr" rid="B96">2014</xref>). Diagonal structures are also linked with a real-life notion of stability (Marwan, <xref ref-type="bibr" rid="B58">2011</xref>; Webber and Marwan, <xref ref-type="bibr" rid="B96">2014</xref>). Consider two points in phase space that start as close neighbors and are followed over time. The length of the diagonal line represents the time that these points remain close (Figures <xref ref-type="fig" rid="F1">1C,D</xref>, dark and light green CoP motion example). The initial distance between the neighboring points at the start could be viewed as a small perturbation, i.e., a small difference in initial conditions, and the length of the diagonal line reflects whether balance control is affected by these small perturbations. Longer diagonal lines indicate balance control that is minimally affected by these small perturbations. Balance control must deal with these small perturbations to remain stable as upright stance can be viewed as an inverted pendulum which is inherently unstable due to its physics. Therefore, diagonal line features reflect the performance in dealing with small perturbations, the longer the diagonal line lengths are, the better the performance of balance control. In contrast, lower percentage determinism and shorter mean diagonal line length would reflect less predictable (i.e., more sensitive to small perturbations, lower balance performance) and more random CoP motion.</p>
<p><italic>Vertical line features</italic>. Vertical line features reflect intermittent (laminar) behavior of CoP motion (Figures <xref ref-type="fig" rid="F1">1C,D</xref>). The percentage of recurrences that form vertical lines (%LAM) and the mean vertical line length (TT) measures intermittent behavior of CoP motion. Intermittent behavior reflects CoP motion that now and again exhibits changes in CoP dynamics from fluctuating to relatively stationary. For example, a vertical line occurs when a balance solution (state) revisits (Figures <xref ref-type="fig" rid="F1">1C,D</xref>, red dot CoP position example) a region in phase space, but then remains in that region for some time (Figures <xref ref-type="fig" rid="F1">1C,D</xref>, red line CoP motion example). A period of minimal change in balance states reflects balance that did not require substantial corrections during that time period. The length of these time periods, as measured by TT, reflects the presence of a point attractor, presumably a stable static state. Low laminarity and shorter mean vertical line lengths reflect balance control with fewer static states.</p>
<p><italic>Detrended fluctuation analysis</italic>. DFA measures the long-range dependence in signals, also referred to as &#x0201C;memory&#x0201D; (Peng et al., <xref ref-type="bibr" rid="B67">1998</xref>). DFA measures the exponential relation between CoP fluctuations at different time windows (time scales) by measuring the slope of a linear region on the log-log plot of CoP fluctuations vs. time scales (Figure <xref ref-type="fig" rid="F2">2</xref>). The slope reveals the general organization of these fluctuations across a range of time scales. For example, a steeper slope of the exponential relation between CoP fluctuations at different time scales reflects CoP motion in which relative contribution of fluctuations at shorter time scales are less than fluctuations at longer time scales or vise versa. With this particular organization of fluctuations across the timescales, CoP motion appears to be smoother and tends to continue to move (persist) in the same direction (Mandelbrot, <xref ref-type="bibr" rid="B56">1982</xref>), reflecting CoP motion that did not involve many direction changes. Figure <xref ref-type="fig" rid="F2">2</xref> shows the technical details and settings of the used DFA method, and Table <xref ref-type="table" rid="T1">1</xref> provides definition and interpretations of DFA parameters used in the current study.</p>
<fig id="F2" position="float">
<label>Figure 2</label>
<caption><p>Detrended fluctuation analysis (DFA) methods. <bold>(A)</bold> Example of a 15-s CoP motion (see Figure <xref ref-type="fig" rid="F1">1A</xref> in blue). <bold>(B)</bold> CoP was integrated, then fluctuations of CoP around linear fits over windows ranging from 0.10 to 4.42 s were determined with 50% overlap. Example of 0.2 s is given. <bold>(C)</bold> Log-log plot of time windows vs. fluctuations. Two linear regions were fit by minimizing the squared errors between the combined linear fits and actual data. DFA<sub>1</sub> and DFA<sub>2</sub> reflect the general organization of fluctuations at shorter and longer time scales, respectively. DFA<sub>tau</sub> reflects the time scale between DFA<sub>1</sub> and DFA<sub>2</sub>.</p></caption>
<graphic xlink:href="fphys-09-00273-g0002.tif"/>
</fig>
<p>Briefly, the CoP signal was integrated over time to allow assessment of fluctuations at longer time scales (Deligni&#x000E8;res et al., <xref ref-type="bibr" rid="B20">2010</xref>). The signal was then divided into smaller time windows with 50% overlap. In each time window, the linear trend was subtracted and the RMS fluctuations of the integrated CoP around the linear fits were determined. The window sizes ranged from 0.10 to 4.42 s. DFA has similarities with spectral analysis (Buldyrev et al., <xref ref-type="bibr" rid="B11">1995</xref>), fluctuations within each window represent fluctuations at a frequency that can be captured within the time window of interest. Therefore, fluctuations within the 0.10&#x02013;4.42 s windows represent fluctuations at frequencies ranging from 10 to 0.23 Hz. The underlying assumption is that CoP motion reflects a form of Brownian motion, and whether Brownian motion is persistent or anti-persistent is reflected by the slope of the fluctuations across multiple time scales (slope: anti-persistent &#x0003C;0.5&#x02013;&#x0003E;0.5 persistent). However, although Brownian motion and non-stationary processes do not need to be integrated over time (Riley et al., <xref ref-type="bibr" rid="B76">2012</xref>) as they are unbounded (i.e., Brownian motion is the integrated form of fractal Gaussian motion), it is beneficial to integrate CoP motion over time to allow assessment of fluctuations at larger time scales because CoP motion is bounded by the support surface area. However, because CoP motion is bounded and non-stationary, integration will consequently inflate the slope of the log-log plot of time-scales vs. fluctuations (Riley et al., <xref ref-type="bibr" rid="B76">2012</xref>). Therefore, the slope will be interpreted like integrated Brownian motion. When the slope &#x0003E;1.5, a change in CoP movement is likely to be followed by a change in the same direction (CoP is persistent). If the slope alpha &#x0003C;1.5, a change in CoP motion is likely to be followed by a change in the opposite direction (CoP is anti-persistent). If alpha &#x0003D; 1.5, then a change in direction of CoP motion does not depend on previous directional changes, and relative contributions of fluctuations at different time scales are equal. Inspection of the log-log plot of time scale vs. fluctuations revealed a bilinear pattern (Figure <xref ref-type="fig" rid="F2">2</xref>). Hence, we calculated the slopes at shorter (DFA<sub>1</sub>) and longer (DFA<sub>2</sub>) time scales and the time point that marked the boundary between the two regions (DFA<sub>tau</sub>). The slope (DFA<sub>2</sub>) of the second region was in general smaller than 1.5, indicating that fluctuations at these time scales reflected CoP motion that tends to turn back toward the point it came from. Consequently, DFA<sub>tau</sub> reflects the time scale at which persistent CoP motion changes into anti-persistent motion. Smooth COP dynamics, without large corrections, would be represented by a greater DFA<sub>1</sub>, DFA<sub>2</sub>, and DFA<sub>tau</sub>. A shorter DFA<sub>tau</sub> and lower DFA<sub>2</sub> values would reflect a more conservative balance strategy with early and strong CoP corrections.</p>
<p>The bi-linear pattern was determined as follows; two linear regions were fit on the log-log plot of time scales vs. fluctuations data by minimizing the squared errors between the combined linear fits and actual data. The region of the first linear fit (shorter time scales) was defined as DFA<sub>1</sub> and the region of the second linear fit (longer time scales) was defined as DFA<sub>2</sub>. The time point separating these two linear regions was defined as DFA<sub>tau</sub>.</p>
</sec>
</sec>
</sec>
<sec>
<title>Statistics</title>
<p>Matlab was used to perform the statistical analysis. The threshold for significance was set at <italic>P</italic> &#x0003C; 0.05.</p>
<sec>
<title>Demographics</title>
<p>Differences between the demographics and PPA of the fallers and non-fallers were assessed using dependent <italic>t</italic>-tests and Chi<sup>2</sup> for sex.</p>
</sec>
<sec>
<title>CoP motion at baseline</title>
<p>Differences between groups at baseline (15 s epoch before vibration) for each outcome variable (linear and non-linear) were assessed using one-way analysis of variance (ANOVA). <italic>Post-hoc</italic> analysis was performed as appropriate with Bonferonni correction for multiple comparisons.</p>
</sec>
<sec>
<title>CoP motion during and after vibration</title>
<p>Differences between fallers, non-fallers, and young for each of the non-linear and linear outcome measures were tested using a wavelet based linear mixed models (adapted from McKay et al., <xref ref-type="bibr" rid="B61">2013</xref>). Wavelet based compression of the data reduces the number of significant <italic>P</italic>-values and therefore increases the statistical power (McKay et al., <xref ref-type="bibr" rid="B61">2013</xref>). Briefly, data from the windowed analysis including two repetitions (2 &#x000D7; 32 data points) for each participant of the vibration epoch and the post vibration epochs (Figure <xref ref-type="fig" rid="F1">1A</xref>), were subjected to a level 1 wavelet transform using the Haar wavelet with periodic extension. For each wavelet coefficient, a linear mixed model was applied to assess differences between groups. Group and repetition were entered as fixed factors and participants were entered as random factors in the linear mixed model. Coefficients reflecting the differences between groups (young vs. non-fallers, young vs. fallers, and fallers vs. non-fallers) were assessed and corresponding <italic>P</italic>-values were stored. All <italic>P</italic>-values were then corrected for multiple comparisons using the Benjamini&#x02013;Hochberg false discovery rate procedure (Benjamini and Hochberg, <xref ref-type="bibr" rid="B7">1995</xref>). Wavelet coefficients representing significant group differences were then transformed back into the time domain.</p>
</sec>
</sec>
</sec>
<sec sec-type="results" id="s3">
<title>Results</title>
<sec>
<title>Falls incidence</title>
<p>Four elderly participants withdrew from the study (1 &#x0003C; 0.5 PPA, and 3 &#x0003E; 1.16 PPA), and no prospective falls data were available for these participants. Forty-two out of 102 elderly participants reported 1 or more falls. Of these participants, 2 reported 6 falls, 1 reported 5 falls, 3 reported 4 falls, 6 reported 3 falls, 9 reported 2 falls, and 21 participants reported 1 fall. Using the prospective falls data, the elderly were grouped into fallers (1 or more prospective falls) and non-fallers. Due to technical issues with data collection, data from 3 participants (1 faller and 2 non-fallers) were excluded from further analysis. Table <xref ref-type="table" rid="T2">2</xref> shows means (SD) of demographics and PPA values of all elderly participants included in the final analysis (<italic>n</italic> &#x0003D; 99). Age, height, weight, sex, and PPA values did not differ significantly between fallers and non-fallers (all, <italic>P</italic> &#x0003E; 0.09, Table <xref ref-type="table" rid="T2">2</xref>).</p>
<table-wrap position="float" id="T2">
<label>Table 2</label>
<caption><p>Participant demographics.</p></caption>
<table frame="hsides" rules="groups">
<thead><tr>
<th/>
<th valign="top" align="center"><bold>n</bold></th>
<th valign="top" align="center"><bold>Height (m)</bold></th>
<th valign="top" align="center"><bold>Weight (kg)</bold></th>
<th valign="top" align="center"><bold>Age (years)</bold></th>
<th valign="top" align="center"><bold>Gender</bold></th>
<th valign="top" align="center"><bold>PPA</bold></th>
</tr>
</thead>
<tbody>
<tr>
<td valign="top" align="left">Fallers</td>
<td valign="top" align="center">41</td>
<td valign="top" align="center">1.70 (0.08)</td>
<td valign="top" align="center">78 (17)</td>
<td valign="top" align="center">76 (5)</td>
<td valign="top" align="center">13 &#x02640;, 28 &#x02642;</td>
<td valign="top" align="center">0.86 (1.00)</td>
</tr>
<tr>
<td valign="top" align="left">Non-fallers</td>
<td valign="top" align="center">58</td>
<td valign="top" align="center">1.68 (0.10)</td>
<td valign="top" align="center">79 (15)</td>
<td valign="top" align="center">75 (6)</td>
<td valign="top" align="center">27 &#x02640;, 31 &#x02642;</td>
<td valign="top" align="center">0.52 (1.00)</td>
</tr>
<tr>
<td valign="top" align="left"><italic>P</italic>-value</td>
<td/>
<td valign="top" align="center">0.26</td>
<td valign="top" align="center">0.79</td>
<td valign="top" align="center">0.51</td>
<td valign="top" align="center">0.14</td>
<td valign="top" align="center">0.09</td>
</tr>
<tr>
<td valign="top" align="left">Young</td>
<td valign="top" align="center">23</td>
<td valign="top" align="center">1.73 (0.5)</td>
<td valign="top" align="center">66.6 (11.3)</td>
<td valign="top" align="center">21.1 (1.5)</td>
<td valign="top" align="center">15 &#x02640;, 9 &#x02642;</td>
<td/>
</tr>
</tbody>
</table>
<table-wrap-foot>
<p><italic>Data are presented as mean &#x000B1; standard deviation, probability (P) of independent 2-tailed t-tests (Chi<sup>2</sup> for gender) between fallers and non-fallers are shown. &#x02640; represents female, and &#x02642; represents male</italic>.</p>
</table-wrap-foot>
</table-wrap>
</sec>
<sec>
<title>CoP motion at baseline</title>
<p>Results of the one-way ANOVA are presented in Table <xref ref-type="table" rid="T3">3</xref>. At baseline (before vibration), compared to fallers, young had lower SP (moved slower), lower %DET (were more predictable), had longer L<sub>mean</sub> (less sensitive to small perturbations, i.e., better balance performance) and had higher %LAM with longer TT (were more intermittent, with longer static episodes). Regarding DFA analysis, compared to fallers, young exhibited a larger DFA<sub>tau</sub> and DFA<sub>2</sub> (a less conservative balance control strategy, lower anti-persistence: young&#x0003E;fallers) and had a larger DFA<sub>1</sub> (smoother and more persistent: young&#x0003E;fallers). Compared to non-fallers, young also had lower SP (moved slower), longer L<sub>mean</sub>, longer TT, and were less anti-persistent (DFA<sub>2</sub>: young&#x0003C;non-fallers), but %DET, %LAM, DFA<sub>1</sub>, and DFA<sub>tau</sub> were not significantly different between young and non-fallers.</p>
<table-wrap position="float" id="T3">
<label>Table 3</label>
<caption><p>One-way analysis of variance between young (y), fallers (f) and non-fallers (nf) at baseline.</p></caption>
<table frame="hsides" rules="groups">
<thead><tr>
<th/>
<th valign="top" align="left" colspan="5" style="border-bottom: thin solid #000000;"><bold>Oneway ANOVA</bold></th>
<th valign="top" align="center" colspan="3" style="border-bottom: thin solid #000000;"><italic><bold>post-hoc</bold></italic></th>
</tr>
</thead>
<tbody>
<tr>
<td/>
<td/>
<td/>
<td valign="top" align="center" colspan="3" style="border-bottom: thin solid #000000;"><bold>Mean (95% CI)</bold></td>
<td valign="top" align="center" colspan="3" style="border-bottom: thin solid #000000;"><italic><bold>P</bold></italic><bold>-value</bold></td>
</tr>
<tr>
<td valign="top" align="left"><bold>Variable</bold></td>
<td valign="top" align="left"><bold>F</bold></td>
<td valign="top" align="left"><italic><bold>P</bold></italic></td>
<td valign="top" align="left"><bold>y</bold></td>
<td valign="top" align="left"><bold>f</bold></td>
<td valign="top" align="left"><bold>nf</bold></td>
<td valign="top" align="left"><bold>y-f</bold></td>
<td valign="top" align="left"><bold>y-nf</bold></td>
<td valign="top" align="left"><bold>f-nf</bold></td>
</tr> <tr>
<td valign="top" align="left">SP (mm)</td>
<td valign="top" align="left">14.08</td>
<td valign="top" align="left"><bold>0.000</bold></td>
<td valign="top" align="left">6.71 (3.33)</td>
<td valign="top" align="left">14.91 (13.02)</td>
<td valign="top" align="left">14.03 (14.01)</td>
<td valign="top" align="left"><bold>0.000</bold></td>
<td valign="top" align="left"><bold>0.000</bold></td>
<td valign="top" align="left">0.869</td>
</tr>
<tr>
<td valign="top" align="left">%DET</td>
<td valign="top" align="left">5.85</td>
<td valign="top" align="left"><bold>0.004</bold></td>
<td valign="top" align="left">0.91 (0.09)</td>
<td valign="top" align="left">0.86 (0.15)</td>
<td valign="top" align="left">0.88 (0.11)</td>
<td valign="top" align="left"><bold>0.003</bold></td>
<td valign="top" align="left">0.172</td>
<td valign="top" align="left">0.128</td>
</tr>
<tr>
<td valign="top" align="left">L<sub>mean</sub></td>
<td valign="top" align="left">12.89</td>
<td valign="top" align="left"><bold>0.000</bold></td>
<td valign="top" align="left">39.49 (16.01)</td>
<td valign="top" align="left">30.28 (12.02)</td>
<td valign="top" align="left">32.64 (14.03)</td>
<td valign="top" align="left"><bold>0.000</bold></td>
<td valign="top" align="left"><bold>0.000</bold></td>
<td valign="top" align="left">0.275</td>
</tr>
<tr>
<td valign="top" align="left">%LAM</td>
<td valign="top" align="left">7.05</td>
<td valign="top" align="left"><bold>0.001</bold></td>
<td valign="top" align="left">0.95 (0.06)</td>
<td valign="top" align="left">0.88 (0.17)</td>
<td valign="top" align="left">0.91 (0.12)</td>
<td valign="top" align="left"><bold>0.001</bold></td>
<td valign="top" align="left">0.065</td>
<td valign="top" align="left">0.142</td>
</tr>
<tr>
<td valign="top" align="left">TT</td>
<td valign="top" align="left">13.80</td>
<td valign="top" align="left"><bold>0.000</bold></td>
<td valign="top" align="left">35.91 (17.57)</td>
<td valign="top" align="left">24.88 (14.05)</td>
<td valign="top" align="left">27.55 (16.68)</td>
<td valign="top" align="left"><bold>0.000</bold></td>
<td valign="top" align="left"><bold>0.000</bold></td>
<td valign="top" align="left">0.299</td>
</tr>
<tr>
<td valign="top" align="left">DFA<sub>1</sub></td>
<td valign="top" align="left">4.05</td>
<td valign="top" align="left"><bold>0.020</bold></td>
<td valign="top" align="left">1.81 (0.10)</td>
<td valign="top" align="left">1.74 (0.22)</td>
<td valign="top" align="left">1.77 (0.17)</td>
<td valign="top" align="left"><bold>0.017</bold></td>
<td valign="top" align="left">0.290</td>
<td valign="top" align="left">0.280</td>
</tr>
<tr>
<td valign="top" align="left">DFA<sub>2</sub></td>
<td valign="top" align="left">6.35</td>
<td valign="top" align="left"><bold>0.002</bold></td>
<td valign="top" align="left">1.31 (0.40)</td>
<td valign="top" align="left">1.10 (0.46)</td>
<td valign="top" align="left">1.14 (0.47)</td>
<td valign="top" align="left"><bold>0.002</bold></td>
<td valign="top" align="left"><bold>0.011</bold></td>
<td valign="top" align="left">0.792</td>
</tr>
<tr>
<td valign="top" align="left">DFA<sub>tau</sub></td>
<td valign="top" align="left">3.52</td>
<td valign="top" align="left"><bold>0.033</bold></td>
<td valign="top" align="left">0.95 (0.83)</td>
<td valign="top" align="left">0.72 (0.55)</td>
<td valign="top" align="left">0.77 (0.65)</td>
<td valign="top" align="left"><bold>0.033</bold></td>
<td valign="top" align="left">0.087</td>
<td valign="top" align="left">0.890</td>
</tr>
</tbody>
</table>
<table-wrap-foot>
<p><italic>Significant differences are shown in bold font. Recurrence quantification analysis (RQA), diagonal line structures; percentage determinism (%DET), mean diagonal line length (L<sub>mean</sub>), vertical line structure; percentage laminarity (%LAM), mean vertical line length (trapping time, TT). Detrended fluctuation analysis (DFA), short term DFA (DFA<sub>1</sub>), longer term DFA (DFA<sub>2</sub>), and the time scale that separates DFA<sub>1</sub> and DFA<sub>2</sub>; DFA<sub>tau.</sub></italic></p>
</table-wrap-foot>
</table-wrap>
<p>No differences between fallers and non-fallers were observed at baseline.</p>
</sec>
<sec>
<title>CoP motion during and after vibration</title>
<p>Outcome data for CoP motion during and after vibration are shown in Figures <xref ref-type="fig" rid="F3">3</xref>&#x02013;<bold>6</bold>, and summarized in Table <xref ref-type="table" rid="T4">4</xref>. CoP mean displacement relative to baseline in response to calf vibration was not significantly different between the groups (Figure <xref ref-type="fig" rid="F3">3</xref>). In addition, CoP displacement after vibration was also not significantly different between the groups (Figure <xref ref-type="fig" rid="F3">3</xref>, Table <xref ref-type="table" rid="T4">4</xref>).</p>
<fig id="F3" position="float">
<label>Figure 3</label>
<caption><p>Results of linear measures during vibration (VIB) and post-vibration epochs. Top panel show mean for each group of <bold>(A)</bold> mean center of pressure (CoP) displacement and <bold>(B)</bold> sway path length (SP). Bottom panel in <bold>(A,B)</bold> show mean differences between groups (open dots), and the significant (sign) difference between groups (solid lines). Note that group differences are significant when the solid line matches the open dots. Group differences at baseline (BL) were assessed separately and are presented for visual reference. Error bars represent 95% confidence interval (1.96 &#x000D7; standard error of measurement).</p></caption>
<graphic xlink:href="fphys-09-00273-g0003.tif"/>
</fig>
<table-wrap position="float" id="T4">
<label>Table 4</label>
<caption><p>Overview of CoP variables that were different between young, fallers, and non-fallers.</p></caption>
<table frame="hsides" rules="groups">
<thead><tr>
<th/>
<th/>
<th valign="top" align="center" colspan="2" style="border-bottom: thin solid #000000;"><bold>Young vs. fallers</bold></th>
<th valign="top" align="center" colspan="2" style="border-bottom: thin solid #000000;"><bold>Young vs. non-fallers</bold></th>
<th valign="top" align="center" colspan="2" style="border-bottom: thin solid #000000;"><bold>Fallers vs. non-fallers</bold></th>
</tr>
<tr>
<th valign="top" align="left"><bold>Measure</bold></th>
<th valign="top" align="left"><bold>Variable</bold></th>
<th valign="top" align="left"><bold>VIB</bold></th>
<th valign="top" align="left"><bold>Post VIB</bold></th>
<th valign="top" align="left"><bold>VIB</bold></th>
<th valign="top" align="left"><bold>Post VIB</bold></th>
<th valign="top" align="left"><bold>VIB</bold></th>
<th valign="top" align="left"><bold>Post VIB</bold></th>
</tr>
</thead>
<tbody>
<tr>
<td valign="top" align="left">Linear</td>
<td valign="top" align="left">Displacement</td>
<td valign="top" align="left">NS</td>
<td valign="top" align="left">NS</td>
<td valign="top" align="left">NS</td>
<td valign="top" align="left">NS</td>
<td valign="top" align="left">NS</td>
<td valign="top" align="left">NS</td>
</tr>
<tr>
<td/>
<td valign="top" align="left">SP</td>
<td valign="top" align="left">Y&#x0003E;F</td>
<td valign="top" align="left">Y&#x0003E;F all epochs</td>
<td valign="top" align="left">Y&#x0003E;NF</td>
<td valign="top" align="left">Y&#x0003E;NF all epochs</td>
<td valign="top" align="left">NS</td>
<td valign="top" align="left">NS</td>
</tr>
<tr>
<td valign="top" align="left">RQA diagonal</td>
<td valign="top" align="left">%DET</td>
<td valign="top" align="left">Y&#x0003E;F</td>
<td valign="top" align="left">Y&#x0003E;F all epochs</td>
<td valign="top" align="left">Y&#x0003E;NF</td>
<td valign="top" align="left">Y&#x0003E;NF all epochs</td>
<td valign="top" align="left">NS</td>
<td valign="top" align="left">F&#x0003C;NF at epoch 2&#x02013;9</td>
</tr>
<tr>
<td/>
<td valign="top" align="left">L<sub>mean</sub></td>
<td valign="top" align="left">Y&#x0003E;F</td>
<td valign="top" align="left">Y&#x0003E;F all epochs</td>
<td valign="top" align="left">Y&#x0003E;NF</td>
<td valign="top" align="left">Y&#x0003E;NF all epochs</td>
<td valign="top" align="left">NS</td>
<td valign="top" align="left">NS</td>
</tr>
<tr>
<td valign="top" align="left">RQA vertical</td>
<td valign="top" align="left">%LAM</td>
<td valign="top" align="left">Y&#x0003E;F</td>
<td valign="top" align="left">Y&#x0003E;F all epochs</td>
<td valign="top" align="left">Y&#x0003E;NF</td>
<td valign="top" align="left">Y&#x0003E;NF all epochs</td>
<td valign="top" align="left">NS</td>
<td valign="top" align="left">F&#x0003C;NF at epoch 2&#x02013;7</td>
</tr>
<tr>
<td/>
<td valign="top" align="left">TT</td>
<td valign="top" align="left">Y&#x0003E;F</td>
<td valign="top" align="left">Y&#x0003E;F all epochs</td>
<td valign="top" align="left">Y&#x0003E;NF</td>
<td valign="top" align="left">Y&#x0003E;NF all epochs</td>
<td valign="top" align="left">NS</td>
<td valign="top" align="left">NS</td>
</tr>
<tr>
<td valign="top" align="left">DFA</td>
<td valign="top" align="left">DFA short</td>
<td valign="top" align="left">NS</td>
<td valign="top" align="left">Y&#x0003E;F at epochs 2&#x02013;31</td>
<td valign="top" align="left">NS</td>
<td valign="top" align="left">Y&#x0003E;NF at epochs 2&#x02013;27</td>
<td valign="top" align="left">NS</td>
<td valign="top" align="left">F&#x0003C;NF at epochs 2&#x02013;11, 28&#x02013;31</td>
</tr>
<tr>
<td/>
<td valign="top" align="left">DFA long</td>
<td valign="top" align="left">NS</td>
<td valign="top" align="left">Y&#x0003E;F at epochs 6&#x02013;11, 22&#x02013;27, 30, 31</td>
<td valign="top" align="left">NS</td>
<td valign="top" align="left">Y&#x0003E;NF at epochs 6&#x02013;9</td>
<td valign="top" align="left">NS</td>
<td valign="top" align="left">NS</td>
</tr>
<tr>
<td/>
<td valign="top" align="left">DFA tau</td>
<td valign="top" align="left">Y&#x0003E;F</td>
<td valign="top" align="left">Y&#x0003E;F at epochs 1, 2, 11&#x02013;31</td>
<td valign="top" align="left">Y&#x0003E;NF</td>
<td valign="top" align="left">Y&#x0003E;NF at epochs 11&#x02013;31</td>
<td valign="top" align="left">NS</td>
<td valign="top" align="left">NS</td>
</tr>
</tbody>
</table>
<table-wrap-foot>
<p><italic>Recurrence quantification analysis (RQA), diagonal line structures; percentage determinism (%DET), mean diagonal line length (L<sub>mean</sub>), vertical line structure; percentage laminarity (%LAM), mean vertical line length (trapping time, TT). Detrended fluctuation analysis (DFA), short term DFA (DFA<sub>1</sub>), longer term DFA (DFA<sub>2</sub>) and the time scale that separates DFA<sub>1</sub> and DFA<sub>2</sub>; DFA<sub>tau.</sub></italic></p>
</table-wrap-foot>
</table-wrap>
<p>For the young group, compared to fallers and non-fallers, across all epochs, %DET and L<sub>mean</sub> (balance performance; young&#x0003E;fallers/non-fallers, Figure <xref ref-type="fig" rid="F4">4</xref>), %LAM and TT (intermittent control; young&#x0003E;fallers/non-fallers, Figure <xref ref-type="fig" rid="F5">5</xref>), and DFA<sub>1</sub> (smoothness/persistence; young&#x0003E;fallers/non-fallers at most epochs, Figure <xref ref-type="fig" rid="F6">6</xref>) values were higher, and SP (young&#x0003C;fallers/non-fallers, Figure <xref ref-type="fig" rid="F3">3</xref>) was lower (Table <xref ref-type="table" rid="T4">4</xref>). DFA<sub>2</sub> was greater in the young than both fallers and non-fallers after removal of vibration at most epochs (Figure <xref ref-type="fig" rid="F6">6</xref>, Table <xref ref-type="table" rid="T4">4</xref>). DFA<sub>tau</sub> was higher in the young during vibration than both fallers and non-fallers, but, was similar for all groups directly after removal of vibration. DFA<sub>tau</sub> values were higher in the young than both fallers and non-fallers after epoch 12 (Figure <xref ref-type="fig" rid="F6">6</xref>). This suggests that during vibration young were more persistent across more time-scales compared to both fallers and non-fallers (DFA<sub>tau</sub>: young&#x0003E;fallers/non-fallers).</p>
<fig id="F4" position="float">
<label>Figure 4</label>
<caption><p>Results of recurrence quantification analysis (RQA) of diagonal line features during vibration (VIB) and post-vibration epochs. Top panels show mean for each group of <bold>(A)</bold>, mean percentage determinism (%DET) and <bold>(B)</bold> mean diagonal line lengths (L<sub>mean</sub>). Bottom panels in <bold>(A,B)</bold> show mean differences between groups (open dots), and the significant (sign) difference between groups (solid lines). Note that group differences are significant when the solid line matches the open dots. Group differences at baseline (BL) were assessed separately and are presented for visual reference. Error bars represent 95% confidence interval (1.96 &#x000D7; standard error of measurement).</p></caption>
<graphic xlink:href="fphys-09-00273-g0004.tif"/>
</fig>
<fig id="F5" position="float">
<label>Figure 5</label>
<caption><p>Results of recurrence quantification analysis (RQA) of vertical line features during vibration (VIB) and post-vibration epochs. Top panels show mean for each group of <bold>(A)</bold> mean percentage laminarity (%LAM) and <bold>(B)</bold> mean vertical line lengths (TT). Bottom panels in <bold>(A,B)</bold>, mean differences between groups (open dots), and the significant (sign) difference between groups (solid lines). Note that group differences are significant when the solid line matches the open dots. Group differences at baseline (BL) were assessed separately and are presented for visual reference. Error bars represent 95% confidence interval (1.96 &#x000D7; standard error of measurement).</p></caption>
<graphic xlink:href="fphys-09-00273-g0005.tif"/>
</fig>
<fig id="F6" position="float">
<label>Figure 6</label>
<caption><p>Results of detrended fluctuation analysis (DFA) during vibration (VIB) and post-vibration epochs. Top panels show mean for each group of <bold>(A)</bold> DFA<sub>1</sub> (short term), <bold>(B)</bold> DFA<sub>2</sub> (long term), and <bold>(C)</bold> DFA<sub>tau</sub> (time scale that separates DFA<sub>1</sub> and DFA<sub>2</sub>). Bottom panels in <bold>(A&#x02013;C)</bold> show mean differences between groups (open dots), and the significant (sign) difference between groups (solid lines). Note that group differences are significant when the solid line matches the open dots. Group differences at baseline (BL) were assessed separately and are presented for visual reference. Error bars represent 95% confidence interval (1.96 &#x000D7; standard error of measurement).</p></caption>
<graphic xlink:href="fphys-09-00273-g0006.tif"/>
</fig>
<p>During ankle vibration, fallers and non-fallers were not significantly different in any of the linear or non-linear outcome variables (Figures <xref ref-type="fig" rid="F3">3</xref>&#x02013;<xref ref-type="fig" rid="F6">6</xref>). However, after removal of ankle vibration, CoP motion of the fallers had lower %DET (less predictable/more random; fallers&#x0003C;non-fallers, Figure <xref ref-type="fig" rid="F4">4</xref>), lower %LAM (less intermittent; fallers&#x0003C;non-fallers, Figure <xref ref-type="fig" rid="F5">5</xref>), and lower DFA<sub>1</sub> (less smooth/less persistent; Figure <xref ref-type="fig" rid="F6">6</xref>) values than those in non-fallers. See Table <xref ref-type="table" rid="T4">4</xref> for overview of the findings.</p>
</sec>
</sec>
<sec sec-type="discussion" id="s4">
<title>Discussion</title>
<p>This study assessed the effect of addition and removal of calf vibration on balance control (in the absence of vision) in elderly people who did or did not prospectively report falls and a group of young individuals. Mean CoP displacement during and after vibration did not differ between groups, suggesting that peripheral functioning of calf proprioception and weighting assigned by the CNS to calf proprioception were similar for the young and both groups of older individuals. Overall, compared to the elderly, the CoP motion of young was more predictable and less sensitive to small perturbations. Notably, non-linear aspects of CoP motion of fallers differed from that of non-fallers after removal of vibration, a period in which dynamic re-weighting is required (Teasdale and Simoneau, <xref ref-type="bibr" rid="B91">2001</xref>). During this period fallers exhibited more random CoP motion.</p>
<sec>
<title>Interpretation of non-linear measures of CoP motion</title>
<p>Our conclusions are based on interpretation of the non-linear measures of CoP motion, yet alternative interpretations of some RQA measures requires consideration (Negahban et al., <xref ref-type="bibr" rid="B64">2010</xref>; Ramdani et al., <xref ref-type="bibr" rid="B74">2013</xref>; Bernard et al., <xref ref-type="bibr" rid="B8">2015</xref>). In contrast to our interpretation that a more deterministic structure infers more regular and stable balance control, this regularity has also been interpreted to reflect less behavioral flexibility and less complexity in CoP motion. That alternative interpretation was motivated by observations of increased regularity of CoP motion in Parkinson&#x00027;s disease (Schmit et al., <xref ref-type="bibr" rid="B82">2006</xref>), retrospectively identified fallers (Ramdani et al., <xref ref-type="bibr" rid="B74">2013</xref>), and in individuals with anterior cruciate ligament deficiency (Negahban et al., <xref ref-type="bibr" rid="B64">2010</xref>). Although these interpretations might be reasonable in some cases (e.g., Parkinson&#x00027;s Disease), it might not apply to our observations.</p>
<p>Our interpretations and of others (Riley et al., <xref ref-type="bibr" rid="B75">1999</xref>; Riley and Clark, <xref ref-type="bibr" rid="B77">2003</xref>; Haddad et al., <xref ref-type="bibr" rid="B37">2008</xref>; Cluff et al., <xref ref-type="bibr" rid="B17">2009</xref>; Mazaheri et al., <xref ref-type="bibr" rid="B60">2010</xref>) are based on the construct validity of RQA, methodological issues, and the nature and difficulty of our balance task. The deterministic structure is related to diagonal line feature in the recurrence plot. Both %DET and L<sub>mean</sub> reflect CoP motions that run parallel in phase space because different CoP sections are spatially and temporally similar in shape (Figures <xref ref-type="fig" rid="F1">1C,D</xref>). This similarity reflects predictability, regularity and local stability of CoP motion. A lower %DET and shorter L<sub>mean</sub> does not necessarily reflect more complex structure because random signals and noise also exhibit low %DET, yet those signals do not have a complex structure. Thus, although &#x0201C;predictability&#x0201D; can be determined, care is required to interpret &#x0201C;flexibility&#x0201D; and &#x0201C;complexity&#x0201D; from RQA outcome variables.</p>
<p>Interpretation of RQA can be aided by concurrent assessment of other non-linear features using additional measures such as DFA, as we have done. Our observation that young people have higher long-range correlations than elderly concurs with other observations of similar differences between young and old (Norris et al., <xref ref-type="bibr" rid="B66">2005</xref>; Amoud et al., <xref ref-type="bibr" rid="B3">2007</xref>; Duarte and Sternad, <xref ref-type="bibr" rid="B26">2008</xref>; Kim et al., <xref ref-type="bibr" rid="B50">2008</xref>). Observed CoP fluctuations reflect both the perturbations [internal (self-generated) and external] and the postural responses to perturbations. The combination of these perturbations is resolved by the postural system. When the postural system appropriately responds to perturbations, then successive CoP positions relate to previous positions and correlation is strong (Bruijn et al., <xref ref-type="bibr" rid="B9">2013</xref>). Successful balance corrections to perturbations would not likely result in additional changes of CoP direction, but instead induce smooth CoP motion that tends to persist in the same direction. Alternatively, more changes in direction would increase the relative contribution of CoP fluctuations at shorter time-scales (DFA<sub>1</sub>) and reduce the strength of long-range correlations. CoP motion with fewer directional changes/smoother appearance would more likely be more deterministic than CoP with more directional changes. Thus, DFA outcomes aid interpretation of whether the deterministic structure of signals arise from regular signals containing fluctuations at a single or limited number of time scales (such as a sine wave), or from regular signals with long-range correlations across multiple time scales. Taken together, concurrent observations of RQA and DFA strengthen our interpretation that high %DET and long L<sub>mean</sub> observed in CoP motion of the young compared to the elderly is not related to reduced complexity as underlying CoP fluctuations were evident at a range of time scales.</p>
<p>Some RQA settings require consideration as they could impact findings. Without an appropriate corridor (Theiler window, shown in Figure <xref ref-type="fig" rid="F1">1C</xref>) along the line of identity (i.e., self-recurrences of CoP states), diagonal line measures could be overestimated by the inclusion of recurrences that are temporally close (Marwan, <xref ref-type="bibr" rid="B58">2011</xref>). This is important as the threshold, below which a recurrence is defined, depends on the phase space diameter (i.e., the amplitude of CoP movements) or depends on the fixed amount of recurrences in the recurrence plot. In both cases, higher amplitude CoP motion, resulting in a larger phase space diameter, would require a higher recurrence threshold. This would increase the neighborhood to find recurrences. Greater amplitude of CoP motion is usually observed in elderly (Hageman et al., <xref ref-type="bibr" rid="B38">1995</xref>; Gill et al., <xref ref-type="bibr" rid="B32">2001</xref>; Abrahamov&#x000E1; and Hlava&#x0010D;ka, <xref ref-type="bibr" rid="B1">2008</xref>). In these cases, RQA would be biased to observe longer diagonal lines and higher determinism if an appropriate Theiler window was not used (Marwan, <xref ref-type="bibr" rid="B58">2011</xref>) allowing inclusion of temporally close neighbors. We used a 1-s Theiler window to minimize this bias. Use of a Theiler window was not reported in previous studies (Seigle et al., <xref ref-type="bibr" rid="B83">2009</xref>; Ramdani et al., <xref ref-type="bibr" rid="B74">2013</xref>; Bernard et al., <xref ref-type="bibr" rid="B8">2015</xref>), the max diagonal lines reported in some studies (Riley and Clark, <xref ref-type="bibr" rid="B77">2003</xref>; Schmit et al., <xref ref-type="bibr" rid="B82">2006</xref>) generally approach the length of the delay embedded signals, which implies that a Theiler window was not applied and findings may have been biased.</p>
<p>The difficulty of the task used to assess balance control requires consideration. In the current study, participants maintained balance while somatosensory information from the calf muscle was suddenly altered by addition and removal of vibration in the absence of vision. Although aware of the experimental conditions, participants were in an unfamiliar balance situation and none had previously experienced muscle vibration. When balance is challenged, more predictable balance control could be beneficial. Increased regularity and smoothness of CoP motion could be interpreted as an appropriate adaptation to a more challenging balance task (Riley et al., <xref ref-type="bibr" rid="B75">1999</xref>).</p>
</sec>
<sec>
<title>Effect of vibration on postural control</title>
<p>The postural vertical is modified when sensory input is increased by muscle vibration (Eklund, <xref ref-type="bibr" rid="B31">1972</xref>). The impact of vibration depends on both peripheral functioning of the muscle spindles and the weighting of this sensory input. Our results showed, on average, that linear measures of the CoP displacement caused by addition and removal of calf vibration did not differ between the young group and both older groups. This suggests the peripheral functioning of the calf proprioceptors and the weight assigned to the sensory information were not different between the groups. Although, Brumagne et al. (<xref ref-type="bibr" rid="B10">2004</xref>) also found similar CoP displacement for older and healthy young individuals, some authors (Pyykk&#x000F6; et al., <xref ref-type="bibr" rid="B72">1990</xref>; Quoniam et al., <xref ref-type="bibr" rid="B73">1995</xref>) reported less CoP response to calf vibration with increased age. Pyykk&#x000F6; et al. (<xref ref-type="bibr" rid="B72">1990</xref>) and Quoniam et al. (<xref ref-type="bibr" rid="B73">1995</xref>) used older individuals from a non-community dwelling setting which might explain the difference in outcome. Further, Quoniam et al. (<xref ref-type="bibr" rid="B73">1995</xref>) used 3 s vibration (15 s used here), which might be too short (Capic&#x000ED;kov&#x000E1; et al., <xref ref-type="bibr" rid="B14">2006</xref>) to affect their elderly group&#x00027;s CoP.</p>
<p>Although addition of vibration did not differently perturb balance in fallers and non-fallers, removal of the vibratory stimulus revealed differences. This implies that dynamical integration of sensory information is more challenging when sensory input is reduced than when it is augmented. This appears to concur with observations that, in some contexts, addition of a subthreshold stochastic stimulus (e.g., vibration shoe soles) can improve balance (Niemi et al., <xref ref-type="bibr" rid="B65">2002</xref>; Priplata et al., <xref ref-type="bibr" rid="B70">2003</xref>). Although we did not observe improvement of balance in response to sudden unfamiliar addition of a supra-threshold vibratory stimulus to the muscle, our data did show that both fallers and non-fallers responded equally well to this perturbation (across our suite of measures). Spindle activity related to changes in calf muscle length is likely to be masked during vibration (Roll et al., <xref ref-type="bibr" rid="B79">1989</xref>) indicative of reweighting of the calf proprioception by the CNS away from the additional inaccurate component provided by the vibration. Although inaccurate information is provided, the additional input was integrated by the CNS for balance control evident by the backwards CoP shift in all groups. Cessation of vibration ceases the vibration related discharges immediately (Roll et al., <xref ref-type="bibr" rid="B79">1989</xref>). Because the proprioceptive information was down-weighted during vibration, sudden reduction of proprioceptive information may be more difficult to accommodate to than adding proprioceptive information using vibration. The period after removal of vibration would require fast reweighting to use available somatosensory information (van der Kooij and Peterka, <xref ref-type="bibr" rid="B93">2011</xref>) and the proprioceptive information from the calf might contain greater noise (Rogers et al., <xref ref-type="bibr" rid="B78">1985</xref>) and less useful somatosensory information than during vibration. Further, analysis using the sliding window after removal of vibration may have reduced the variance leading to a greater probability to observe significant differences between groups than the analysis of a single epoch during vibration.</p>
<p>SP is known to increase, together with L<sub>mean</sub> and %DET, in balance tasks with greater sensory challenge (e.g., eye closure, compliant surfaces; Riley et al., <xref ref-type="bibr" rid="B75">1999</xref>; Riley and Clark, <xref ref-type="bibr" rid="B77">2003</xref>). Increased sway would generate more proprioceptive information and potentially compensate for reduction/removal of sensory information from other sources (Carpenter et al., <xref ref-type="bibr" rid="B15">2001</xref>, <xref ref-type="bibr" rid="B16">2010</xref>). This &#x0201C;self-generated&#x0201D; proprioceptive information is dynamically integrated to guide balance control leading to more deterministic CoP motion and has been referred to as &#x0201C;perceptually guided control&#x0201D; (Riley et al., <xref ref-type="bibr" rid="B75">1999</xref>). Although our elderly group had longer SP than the young group, this was not associated with more deterministic CoP motion. A similar observation was made by Seigle et al. (<xref ref-type="bibr" rid="B83">2009</xref>); removal of vision in quiet stance led to greater SP but less %DET in elderly than younger individuals. This highlights a potential compromise in perceptually guided control in the elderly; particularly for fallers after removal of vibration.</p>
<p>Lower DFA<sub>2</sub> and DFA<sub>tau</sub> in all groups after vibration removal suggest that fluctuations at longer timescales were relatively small (&#x0007E;&#x0003E;0.8 s from DFA<sub>tau</sub>). Proprioceptive information that establishes sense of upright functions at lower frequencies (Diener et al., <xref ref-type="bibr" rid="B24">1986</xref>; Diener and Dichgans, <xref ref-type="bibr" rid="B23">1988</xref>), and reduced fluctuation at longer time scales could reflect that the vertical upright of the participants was affected after removal of calf vibration. The observation of greater DFA<sub>2</sub> and DFA<sub>tau</sub> for young than older participants after &#x0007E;15 epochs (window starting 15 s after cessation of vibration) suggests that young more successfully established an upright subjective vertical. As we assessed fluctuation at a maximum time scale of 4.42 s our data might partly reflect recalibration of upright sense by dynamic reweighting of sensory information that establishes upright sense (i.e., proprioceptive information from the calf and vestibular input).</p>
<p>Poorer balance control after removal of vibration in fallers might be related to an inferior capacity to dynamically reweight the sources of somatosensory information to minimize the perturbation effects of vibration removal. The ability to flexibly explore somatosensory information is affected by increased age (Teasdale et al., <xref ref-type="bibr" rid="B92">1991</xref>; Hay et al., <xref ref-type="bibr" rid="B43">1996</xref>; Doumas and Krampe, <xref ref-type="bibr" rid="B25">2010</xref>; Eikema et al., <xref ref-type="bibr" rid="B29">2013</xref>, <xref ref-type="bibr" rid="B30">2014</xref>). Reduced functioning of somatosensory systems other than the calf muscle spindles might also affect balance steadiness. Physiological aging affects all somatosensory systems (Sturnieks et al., <xref ref-type="bibr" rid="B88">2008</xref>), particularly the vestibular system (Sloane et al., <xref ref-type="bibr" rid="B86">1989</xref>; Strupp et al., <xref ref-type="bibr" rid="B87">1999</xref>) as evidenced by greater dependence of elderly individuals on visual information to establish vertical upright (Sundermier et al., <xref ref-type="bibr" rid="B89">1996</xref>; Simoneau et al., <xref ref-type="bibr" rid="B85">1999</xref>), and inferior capacity to align themselves with the vertical after being tilted (Menant et al., <xref ref-type="bibr" rid="B62">2012</xref>). Because sensory information from the calf was unreliable and vision was unavailable in the present study, reliance on vestibular information would have been increased. Compromised function of the vestibular system would also render the somatosensory information less useful, as the internal upright reference frame against which somatosensory information is compared (Horak et al., <xref ref-type="bibr" rid="B46">1989</xref>) is less accurate. Accurate sense of vertical in combination with optimal balance control would be expected to produce CoP motion that exhibits periods of minimal CoP movements and high %LAM as observed in the young group. It follows that lower %LAM observed in the older group, and lower %LAM observed post vibration in fallers than non-fallers might reflect a compromise of this combination. Confirmation that %LAM relates to inaccurate upright sense, poorer balance control, or both cannot be derived from the present data and requires further investigation.</p>
</sec>
<sec>
<title>Fractal nature of CoP motion</title>
<sec>
<title>Balance between order and disorder</title>
<p>Deligni&#x000E8;res et al. (<xref ref-type="bibr" rid="B22">2011</xref>) hypothesized that systems exhibiting long range correlations are flexible and adaptable and are more robust. Long range correlations are argued to stem from the collective behavior of multiple components within the system (Peng et al., <xref ref-type="bibr" rid="B68">1995a</xref>) that partially overlap in functionality generating a multi-scaled and hierarchical structure (Deligni&#x000E8;res and Marmelat, <xref ref-type="bibr" rid="B21">2013</xref>). The lack of a characteristic scale would help prevent a single steady state (excessive mode locking) restricting the functional responsiveness of the system (Peng et al., <xref ref-type="bibr" rid="B67">1998</xref>; Goldberger et al., <xref ref-type="bibr" rid="B34">2002</xref>). The relation of fluctuations at the different scales can be assessed with DFA, however, why the sum of these various contributions is scaling is unclear. Systems with long range correlations fall between systems with too strict control exhibiting excessive order, and systems with no control exhibiting disorder (Peng et al., <xref ref-type="bibr" rid="B67">1998</xref>; Deligni&#x000E8;res and Marmelat, <xref ref-type="bibr" rid="B21">2013</xref>). The elderly&#x00027;s CoP motion with weaker long-range correlations in combination with lower %DET than young, could suggest that balance in elderly was less controlled, and more stochastic. This observation was exacerbated in fallers during a period after cessation of calf vibration compared to non-fallers and suggests that fallers&#x00027; balance was more disorderly (i.e., less controlled) than non-fallers during this time period.</p>
</sec>
<sec>
<title>Underlying balance control mechanisms</title>
<p>A wide variety of physiological processes exhibit complex fluctuations that obey scaling laws describing their fractal nature (Goldberger et al., <xref ref-type="bibr" rid="B34">2002</xref>). Most of these physiological processes are affected by pathology and/or physiological aging (Goldberger et al., <xref ref-type="bibr" rid="B34">2002</xref>). Although the origin of these fluctuations is largely unknown, the organization of these fluctuations is not random. Instead, fluctuations exhibit correlations over a wide range of time-scales and can exhibit different multifractal complexity levels (Ivanov et al., <xref ref-type="bibr" rid="B48">2009</xref>) providing information on the underlying control mechanisms (Ashkenazy et al., <xref ref-type="bibr" rid="B5">2002</xref>; Goldberger et al., <xref ref-type="bibr" rid="B34">2002</xref>; Hu et al., <xref ref-type="bibr" rid="B47">2004</xref>; Ivanov et al., <xref ref-type="bibr" rid="B48">2009</xref>). For instance, the heart beat is regulated by the autonomic nervous system and changes in its control affect the variability of the time between beats (Goldberger et al., <xref ref-type="bibr" rid="B34">2002</xref>). Similarly, the complex central control of gait results in complex variability of the time between consecutive gait cycles (Hausdorff et al., <xref ref-type="bibr" rid="B41">1995</xref>). For example, the correlation of stride time variability and fractal complexity reduces with maturation (Hausdorff et al., <xref ref-type="bibr" rid="B42">1999</xref>; Ashkenazy et al., <xref ref-type="bibr" rid="B5">2002</xref>) and is affected by aging and disease (Hausdorff et al., <xref ref-type="bibr" rid="B40">1997</xref>). These alterations are argued to stem from changes of the CNS possibly reflecting stronger or reduced connections between different parts that control walking (Ashkenazy et al., <xref ref-type="bibr" rid="B5">2002</xref>).</p>
<p>Some potential parallels can be drawn between the observation of changes in stride time variability with aging (Hausdorff et al., <xref ref-type="bibr" rid="B40">1997</xref>). Aging is related to a narrowing of the physiological functional range (Rosenberg, <xref ref-type="bibr" rid="B80">1989</xref>; Shaffer and Harrison, <xref ref-type="bibr" rid="B84">2007</xref>) related with a decline in morphology and physiological functioning of the sensory system (Shaffer and Harrison, <xref ref-type="bibr" rid="B84">2007</xref>), central processing of sensory information (Goble et al., <xref ref-type="bibr" rid="B33">2011</xref>), and muscular system (Rosenberg, <xref ref-type="bibr" rid="B80">1989</xref>). The aging process results in structural and functional changes, which limit the responsiveness and flexibility of the balance control system. In line with Ashkenazy et al. (<xref ref-type="bibr" rid="B5">2002</xref>) and Hausdorff et al. (<xref ref-type="bibr" rid="B40">1997</xref>), DFA values in the present study were lower in elderly than young and were lower in fallers than non-fallers after removal of the vibratory stimulus. These observations suggest a simpler structure and function of the underlying control system in elderly individuals, which was amplified after vibration in fallers compared to non-fallers. Future investigation is required to identify the non-linear properties that underlie the correlations in CoP motion fluctuations as measured by DFA. Preferably without external alteration of sensory information and with longer signal durations.</p>
<p>Although the underlying intrinsic control mechanism of a physiological process can be assessed by its fractal structure (Goldberger et al., <xref ref-type="bibr" rid="B34">2002</xref>), DFA analysis of CoP motion assesses balance control strategies and therefore indirectly reflects the intrinsic structure of the underlying control system. Other factors that underpin CoP motion fluctuations could explain DFA observations. Underlying biomechanics of upright stance are reflected in CoP motion. Upright balance is thought to be intermittently controlled (Loram and Lakie, <xref ref-type="bibr" rid="B51">2002</xref>; Vieira et al., <xref ref-type="bibr" rid="B94">2012</xref>). Postural sway is probably continuously monitored but controlled by intermittent burst-like actions of postural muscles (Vieira et al., <xref ref-type="bibr" rid="B94">2012</xref>). In between postural control actions, low amplitude CoP motion reflects the deterministic motion similar to the motion of an inverted pendulum (Asai et al., <xref ref-type="bibr" rid="B4">2009</xref>). Intermittent control of upright balance could potentially explain the different scaling properties of CoP motion. In this view, DFA<sub>1</sub> reflects the smooth persistent motion, consistent with that of an inverted pendulum, and DFA<sub>2</sub> reflects the anti-persistent motion, consistent with intermittent postural corrections to limit center-of-mass within base of support. Elderly exhibited a more conservative balance strategy with less emphasis on persistence, in line with lower %DET, shorter L<sub>mean</sub> and DFA<sub>1</sub> in elderly than young, and more emphasis on anti-persistence in line with lower DFA<sub>2</sub> during a period (&#x0007E;6&#x02013;24 s) after vibration. Altered balance strategy observed in elderly individuals might reflect age-related changes in the intrinsic structure of the underlying control system.</p>
</sec>
</sec>
</sec>
<sec sec-type="conclusions" id="s5">
<title>Conclusion</title>
<p>The present results show that non-linear measures of CoP motion, in response to a perturbation that challenges reweighting of integration of sensory input, reveal differences in the quality of balance control between young and old individuals and between older individuals who do and do not go on to fall. Consideration of the interpretation of non-linear measures provides new insights into the possible mechanisms underlying balance dysfunction and risk for falling in older individuals.</p>
</sec>
<sec id="s6">
<title>Ethics statement</title>
<p>All subjects gave written informed consent in accordance with the Declaration of Helsinki. The protocol was approved by the University Human Research Ethics Committee of Queensland University of Technology and by the Medical Research Ethics Committee of The University of Queensland.</p>
</sec>
<sec id="s7">
<title>Author contributions</title>
<p>WvdH: Study design, acquisition of data, data analysis, and interpretation, and drafted the manuscript; GK, JvD, and PH: Study design, data interpretation, and manuscript revision. All authors approved final version of manuscript.</p>
<sec>
<title>Conflict of interest statement</title>
<p>The authors declare that the research was conducted in the absence of any commercial or financial relationships that could be construed as a potential conflict of interest.</p>
</sec>
</sec>
</body>
<back>
<ack><p>The authors acknowledge Dr. Ryan Stafford and Dr. Leanne Hall for help during data collection; Dr. Michael Cole and Ms. Jodi Rippey for participant recruitment, screening, and clinical assessments.</p>
</ack>
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<fn-group>
<fn fn-type="financial-disclosure"><p><bold>Funding.</bold> This study was funded by a project grant (ID443210) and Program Grant (APP1091302) from the National Health and Medical Research Council (NHMRC) of Australia. PH is funded by a Senior Principal Research Fellowship from the NHMRC (APP1102905).</p>
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