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<bibitem type="J">   <ARLID>0444162</ARLID> <utime>20240103210104.7</utime><mtime>20150609235959.9</mtime>   <WOS>000356731300069</WOS> <SCOPUS>84934949836</SCOPUS>  <DOI>10.1073/pnas.1505882112</DOI>           <title language="eng" primary="1">Sample and population exponents of generalized Taylor’s law</title>  <specification> <page_count>16 s.</page_count> <media_type>E</media_type> </specification>   <serial><ARLID>cav_un_epca*0257500</ARLID><ISSN>0027-8424</ISSN><title>Proceedings of the National Academy of Sciences of the United States of America</title><part_num/><part_title/><volume_id>112</volume_id><volume>25 (2015)</volume><page_num>7755-7760</page_num><publisher><place/><name>National Academy of Sciences</name><year/></publisher></serial>    <keyword>fluctuation scaling</keyword>   <keyword>multiplicative growth</keyword>   <keyword>power law</keyword>   <keyword>environmental stochasticity</keyword>   <keyword>Markovian environment</keyword>    <author primary="1"> <ARLID>cav_un_auth*0314085</ARLID> <name1>Giometto</name1> <name2>A.</name2> <country>CH</country>  <share>20</share> </author> <author primary="0"> <ARLID>cav_un_auth*0316935</ARLID> <name1>Formentin</name1> <name2>Marco</name2> <full_dept language="cz">Stochastická informatika</full_dept> <full_dept>Department of Stochastic Informatics</full_dept> <department language="cz">SI</department> <department>SI</department> <institution>UTIA-B</institution> <full_dept>Department of Stochastic Informatics</full_dept>  <share>20</share> <fullinstit>Ústav teorie informace a automatizace AV ČR, v. v. i.</fullinstit> </author> <author primary="0"> <ARLID>cav_un_auth*0317332</ARLID> <name1>Rinaldo</name1> <name2>A.</name2> <country>CH</country>  </author> <author primary="0"> <ARLID>cav_un_auth*0317333</ARLID> <name1>Cohen</name1> <name2>J.</name2> <country>US</country> <share>20</share>  </author> <author primary="0"> <ARLID>cav_un_auth*0317334</ARLID> <name1>Maritan</name1> <name2>A.</name2> <country>IT</country>  <share>20</share> </author>   <source> <url>http://library.utia.cas.cz/separaty/2015/SI/formentin-0444162.pdf</url> </source>        <cas_special> <project> <project_id>GAP201/12/2613</project_id> <agency>GA ČR</agency> <ARLID>cav_un_auth*0291241</ARLID> </project>  <abstract language="eng" primary="1">Taylor’s law (TL) states that the variance V of a nonnegative random variable is a power function of its mean M; i.e., V =aM^b. TL has been verified extensively in ecology, where it applies to population abundance, physics, and other natural sciences. Its ubiquitous empirical verification suggests a context-independent mechanism. Sample exponents b measured empirically via the scaling of sample mean and variance typically cluster around the value b=2. Some theoretical models of population growth, however, predict a broad range of values for the population exponent b pertaining to the mean and variance of population density, depending on details of the growth process. Is the widely reported sample exponent b=2 the result of ecological processes or could it be a statistical artifact? Here, we apply large deviations theory and finite-sample arguments to show exactly that in a broad class of growth models the sample exponent is b=2 regardless of the underlying population exponent.</abstract>     <reportyear>2016</reportyear>  <RIV>BA</RIV>      <num_of_auth>5</num_of_auth>  <inst_support> RVO:67985556 </inst_support>  <permalink>http://hdl.handle.net/11104/0247117</permalink>  <cooperation> <ARLID>cav_un_auth*0316939</ARLID> <name>University of Padova</name> <country>IT</country> </cooperation> <cooperation> <ARLID>cav_un_auth*0316940</ARLID> <name>École Polytechnique Fédérale de Lausanne</name> <country>CH</country> </cooperation> <cooperation> <ARLID>cav_un_auth*0316941</ARLID> <name>The Rockefeller University</name> <country>US</country> </cooperation>  <confidential>S</confidential>          <unknown tag="mrcbT16-e">MULTIDISCIPLINARYSCIENCES</unknown> <unknown tag="mrcbT16-f">10.285</unknown> <unknown tag="mrcbT16-g">1.984</unknown> <unknown tag="mrcbT16-h">8.7</unknown> <unknown tag="mrcbT16-i">1.32197</unknown> <unknown tag="mrcbT16-j">4.682</unknown> <unknown tag="mrcbT16-k">593284</unknown> <unknown tag="mrcbT16-s">6.814</unknown> <unknown tag="mrcbT16-4">Q1</unknown> <unknown tag="mrcbT16-5">9.131</unknown> <unknown tag="mrcbT16-6">3281</unknown> <unknown tag="mrcbT16-7">Q1</unknown> <unknown tag="mrcbT16-B">87.814</unknown> <unknown tag="mrcbT16-C">94.4</unknown> <unknown tag="mrcbT16-D">Q1</unknown> <unknown tag="mrcbT16-E">Q1</unknown> <unknown tag="mrcbT16-P">94.444</unknown> <arlyear>2015</arlyear>       <unknown tag="mrcbU14"> 84934949836 SCOPUS </unknown> <unknown tag="mrcbU34"> 000356731300069 WOS </unknown> <unknown tag="mrcbU63"> cav_un_epca*0257500 Proceedings of the National Academy of Sciences of the United States of America 0027-8424 1091-6490 Roč. 112 č. 25 2015 7755 7760 National Academy of Sciences </unknown> </cas_special> </bibitem>