<?xml version="1.0" encoding="UTF-8"?><!DOCTYPE article  PUBLIC "-//NLM//DTD Journal Publishing DTD v3.0 20080202//EN" "http://dtd.nlm.nih.gov/publishing/3.0/journalpublishing3.dtd"><article xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink" dtd-version="3.0" xml:lang="en" article-type="research article"><front><journal-meta><journal-id journal-id-type="publisher-id">OJS</journal-id><journal-title-group><journal-title>Open Journal of Statistics</journal-title></journal-title-group><issn pub-type="epub">2161-718X</issn><publisher><publisher-name>Scientific Research Publishing</publisher-name></publisher></journal-meta><article-meta><article-id pub-id-type="doi">10.4236/ojs.2015.51007</article-id><article-id pub-id-type="publisher-id">OJS-54078</article-id><article-categories><subj-group subj-group-type="heading"><subject>Articles</subject></subj-group><subj-group subj-group-type="Discipline-v2"><subject>Physics&amp;Mathematics</subject></subj-group></article-categories><title-group><article-title>
 
 
  Combining Likelihood Information from Independent Investigations
 
</article-title></title-group><contrib-group><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>.</surname><given-names>Jiang</given-names></name><xref ref-type="aff" rid="aff1"><sup>1</sup></xref><xref ref-type="corresp" rid="cor1"><sup>*</sup></xref></contrib><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>A.</surname><given-names>Wong</given-names></name><xref ref-type="aff" rid="aff1"><sup>1</sup></xref><xref ref-type="corresp" rid="cor1"><sup>*</sup></xref></contrib></contrib-group><aff id="aff1"><addr-line>Department of Mathematics and Statistics, York University, Toronto, Canada</addr-line></aff><author-notes><corresp id="cor1">* E-mail:<email>august@mathstat.yorku.ca(.J)</email>;<email>august@yorku.ca(AW)</email>;</corresp></author-notes><pub-date pub-type="epub"><day>20</day><month>01</month><year>2015</year></pub-date><volume>05</volume><issue>01</issue><fpage>51</fpage><lpage>59</lpage><history><date date-type="received"><day>23</day>	<month>January</month>	<year>2015</year></date><date date-type="rev-recd"><day>accepted</day>	<month>11</month>	<year>February</year>	</date><date date-type="accepted"><day>15</day>	<month>February</month>	<year>2015</year></date></history><permissions><copyright-statement>&#169; Copyright  2014 by authors and Scientific Research Publishing Inc. </copyright-statement><copyright-year>2014</copyright-year><license><license-p>This work is licensed under the Creative Commons Attribution International License (CC BY). http://creativecommons.org/licenses/by/4.0/</license-p></license></permissions><abstract><p>
 
 
  Fisher [1] proposed a simple method to combine 
  <em>p</em>-values from independent investigations without using detailed information of the original data. In recent years, likelihood-based asymptotic methods have been developed to produce highly accurate 
  <em>p</em>-values. These likelihood-based methods generally required the likelihood function and the standardized maximum likelihood estimates departure calculated in the canonical parameter scale. In this paper, a method is proposed to obtain a 
  <em>p</em>-value by combining the likelihood functions and the standardized maximum likelihood estimates departure of independent investigations for testing a scalar parameter of interest. Examples are presented to illustrate the application of the proposed method and simulation studies are performed to compare the accuracy of the proposed method with Fisher’s method.
 
</p></abstract><kwd-group><kwd>Canonical Parameter</kwd><kwd> Fisher’s Expected Information</kwd><kwd> Modified Signed Log-Likelihood Ratio  Statistic</kwd><kwd> Standardized Maximum Likelihood Estimate Departure</kwd></kwd-group></article-meta></front><body><sec id="s1"><title>1. Introduction</title><p>Supposed that <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-1240445x5.png" xlink:type="simple"/></inline-formula> independent investigations are conducted to test the same null hypothesis and the p-values are <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-1240445x6.png" xlink:type="simple"/></inline-formula> respectively. Fisher [<xref ref-type="bibr" rid="scirp.54078-ref1">1</xref>] proposed a simple method to combine these p-values to obtain a single p-value <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-1240445x7.png" xlink:type="simple"/></inline-formula> without using the detailed information concerning the original data nor knowing how these p-values were obtained. His methodology is based on the following two results from distribution theories:</p><p>1) If <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-1240445x8.png" xlink:type="simple"/></inline-formula> is distributed as Uniform(0, 1), then <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-1240445x9.png" xlink:type="simple"/></inline-formula> is distributed as Chi-square with 2 degrees of freedom <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-1240445x10.png" xlink:type="simple"/></inline-formula></p><p>2) If <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-1240445x11.png" xlink:type="simple"/></inline-formula> are independently distributed as<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-1240445x12.png" xlink:type="simple"/></inline-formula>, then <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-1240445x13.png" xlink:type="simple"/></inline-formula> is distributed as<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-1240445x14.png" xlink:type="simple"/></inline-formula>.</p><p>Since <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-1240445x15.png" xlink:type="simple"/></inline-formula> are independently distributed as Uniform(0, 1), then the combined p-value <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-1240445x16.png" xlink:type="simple"/></inline-formula> is</p><disp-formula id="scirp.54078-formula2442"><label>(1)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/7-1240445x17.png"  xlink:type="simple"/></disp-formula><p>For illustration, Fisher [<xref ref-type="bibr" rid="scirp.54078-ref1">1</xref>] reported the p-values of three independent investigations: 0.145, 0.263 and 0.087. Thus the combined p-value is</p><disp-formula id="scirp.54078-formula2443"><graphic  xlink:href="http://html.scirp.org/file/7-1240445x18.png"  xlink:type="simple"/></disp-formula><p>which gives moderate evidence against the null hypothesis. Fisher [<xref ref-type="bibr" rid="scirp.54078-ref1">1</xref>] described the procedure as a “simple test of the significance of the aggregate”.</p><p>As an illustrative example is the study of rate of arrival. It is common to use a Poisson model to model the number of arrivals over a specific time interval. Let <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-1240445x19.png" xlink:type="simple"/></inline-formula> be the number of arrivals in n consecutive unit time intervals and denote <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-1240445x20.png" xlink:type="simple"/></inline-formula> be the total number of arrivals over the n consecutive unit time intervals. Moreover, let <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-1240445x20.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-1240445x21.png" xlink:type="simple"/></inline-formula> be the rate of arrival in an unit time interval. We observed a total of 14 arrivals over 20 consecutive unit time intervals. In other words, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-1240445x20.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-1240445x21.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-1240445x22.png" xlink:type="simple"/></inline-formula>and we are interested in assessing<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-1240445x20.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-1240445x21.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-1240445x22.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-1240445x23.png" xlink:type="simple"/></inline-formula>. Then the null distribution of <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-1240445x20.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-1240445x21.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-1240445x22.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-1240445x23.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-1240445x24.png" xlink:type="simple"/></inline-formula> is Poisson (20) and, based on the observed<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-1240445x20.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-1240445x21.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-1240445x22.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-1240445x23.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-1240445x24.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-1240445x25.png" xlink:type="simple"/></inline-formula>, the mid-p-value is</p><disp-formula id="scirp.54078-formula2444"><graphic  xlink:href="http://html.scirp.org/file/7-1240445x26.png"  xlink:type="simple"/></disp-formula><p>An alternate way of investigating the rate of arrival over a period of time is by modeling the time to first arrival, T with the exponential model with rate<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-1240445x27.png" xlink:type="simple"/></inline-formula>. We observed<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-1240445x27.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-1240445x28.png" xlink:type="simple"/></inline-formula>, and, again, we are interested in assess- ing<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-1240445x27.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-1240445x28.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-1240445x29.png" xlink:type="simple"/></inline-formula>. Then the null distribution of <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-1240445x27.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-1240445x28.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-1240445x29.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-1240445x30.png" xlink:type="simple"/></inline-formula> is the exponential with rate 1, and, based on the observed<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-1240445x27.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-1240445x28.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-1240445x29.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-1240445x30.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-1240445x31.png" xlink:type="simple"/></inline-formula>, the p-value is</p><disp-formula id="scirp.54078-formula2445"><graphic  xlink:href="http://html.scirp.org/file/7-1240445x32.png"  xlink:type="simple"/></disp-formula><p>By Fisher’s way of combining the p-values, we have</p><disp-formula id="scirp.54078-formula2446"><graphic  xlink:href="http://html.scirp.org/file/7-1240445x33.png"  xlink:type="simple"/></disp-formula><p>which gives strong evidence that <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-1240445x34.png" xlink:type="simple"/></inline-formula> is greater than 1.</p><p>In recent years, many likelihood-based asymptotic methods have been developed to produce highly accurate p-values. In particular, both the Lugannani and Rice’s [<xref ref-type="bibr" rid="scirp.54078-ref2">2</xref>] method and the Barndorff-Nielsen’s [<xref ref-type="bibr" rid="scirp.54078-ref3">3</xref>] [<xref ref-type="bibr" rid="scirp.54078-ref4">4</xref>] method produced p-values which have third-order accuracy, i.e. the rate of convergence is<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-1240445x35.png" xlink:type="simple"/></inline-formula>. Fraser and Reid [<xref ref-type="bibr" rid="scirp.54078-ref5">5</xref>] showed that both methods required the signed log-likelihood ratio statistic and the standardized maximum likelihood estimate departure calculated in the canonical parameter scale. In this paper, we proposed a method to combine likelihood functions and the standardized maximum likelihood estimates departure calculated in the canonical parameter scale obtained from independent investigations to obtain a combined p-value.</p><p>In Section 2, a brief review of the third-order likelihood-based method for a scalar parameter of interest is presented. In Section 3, the relationship between the score variable and the locally defined canonical parameter is determined. Using the results in Section 3, a new way of combining likelihood information is proposed in Section 4. Examples and simulation results are presented in Section 5 and some concluding remarks are recorded in Section 6.</p></sec><sec id="s2"><title>2. Third-Order Likelihood-Based Method for a Scalar Parameter of Interest</title><p>Fraser [<xref ref-type="bibr" rid="scirp.54078-ref6">6</xref>] showed that for a sample <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-1240445x36.png" xlink:type="simple"/></inline-formula> from a canonical exponential family model with log-like- lihood function</p><disp-formula id="scirp.54078-formula2447"><graphic  xlink:href="http://html.scirp.org/file/7-1240445x37.png"  xlink:type="simple"/></disp-formula><p>where</p><disp-formula id="scirp.54078-formula2448"><graphic  xlink:href="http://html.scirp.org/file/7-1240445x38.png"  xlink:type="simple"/></disp-formula><p>and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-1240445x39.png" xlink:type="simple"/></inline-formula> is the scalar canonical parameter of interest. The p-value function <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-1240445x39.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-1240445x40.png" xlink:type="simple"/></inline-formula> can be appro- ximated with third-order accuracy using either the Lugannani and Rice [<xref ref-type="bibr" rid="scirp.54078-ref2">2</xref>] formula</p><disp-formula id="scirp.54078-formula2449"><label>(2)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/7-1240445x41.png"  xlink:type="simple"/></disp-formula><p>or the Barndorff-Nielsen [<xref ref-type="bibr" rid="scirp.54078-ref3">3</xref>] [<xref ref-type="bibr" rid="scirp.54078-ref4">4</xref>] formula</p><disp-formula id="scirp.54078-formula2450"><label>(3)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/7-1240445x42.png"  xlink:type="simple"/></disp-formula><p>where <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-1240445x43.png" xlink:type="simple"/></inline-formula> is the signed log-likelihood ratio statistic</p><disp-formula id="scirp.54078-formula2451"><label>(4)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/7-1240445x44.png"  xlink:type="simple"/></disp-formula><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-1240445x45.png" xlink:type="simple"/></inline-formula>is the standardized maximum likelihood departure calculated in the canonical parameter scale:</p><disp-formula id="scirp.54078-formula2452"><label>(5)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/7-1240445x46.png"  xlink:type="simple"/></disp-formula><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-1240445x47.png" xlink:type="simple"/></inline-formula>is the maximum likelihood estimate of <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-1240445x47.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-1240445x48.png" xlink:type="simple"/></inline-formula> satisfying<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-1240445x47.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-1240445x48.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-1240445x49.png" xlink:type="simple"/></inline-formula>, and</p><disp-formula id="scirp.54078-formula2453"><graphic  xlink:href="http://html.scirp.org/file/7-1240445x50.png"  xlink:type="simple"/></disp-formula><p>is the observed information evaluated at<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-1240445x51.png" xlink:type="simple"/></inline-formula>. Jensen [<xref ref-type="bibr" rid="scirp.54078-ref7">7</xref>] showed that (2) and (3) are asymptotically equivalent up to third-order accuracy. In literature, there exists many applications of these methods, for example, see Bra- zzale et al. [<xref ref-type="bibr" rid="scirp.54078-ref8">8</xref>] .</p><p>Fraser and Reid [<xref ref-type="bibr" rid="scirp.54078-ref5">5</xref>] [<xref ref-type="bibr" rid="scirp.54078-ref9">9</xref>] generalized the methodology to any model with log likelihood function<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-1240445x52.png" xlink:type="simple"/></inline-formula>. They defined the locally defined canonical parameter be</p><disp-formula id="scirp.54078-formula2454"><label>(6)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/7-1240445x53.png"  xlink:type="simple"/></disp-formula><p>where</p><disp-formula id="scirp.54078-formula2455"><label>(7)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/7-1240445x54.png"  xlink:type="simple"/></disp-formula><p>is the rate of change of <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-1240445x55.png" xlink:type="simple"/></inline-formula> with respect to the change of <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-1240445x55.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-1240445x56.png" xlink:type="simple"/></inline-formula> at<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-1240445x55.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-1240445x56.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-1240445x57.png" xlink:type="simple"/></inline-formula>, and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-1240445x55.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-1240445x56.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-1240445x57.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-1240445x58.png" xlink:type="simple"/></inline-formula> is a pivotal quantity. Define <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-1240445x55.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-1240445x56.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-1240445x57.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-1240445x58.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-1240445x59.png" xlink:type="simple"/></inline-formula> be the score variable satisfying</p><disp-formula id="scirp.54078-formula2456"><label>(8)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/7-1240445x60.png"  xlink:type="simple"/></disp-formula><p>with <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-1240445x61.png" xlink:type="simple"/></inline-formula> being the maximum likelihood estimate of <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-1240445x61.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-1240445x62.png" xlink:type="simple"/></inline-formula> obtained from <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-1240445x61.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-1240445x62.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-1240445x63.png" xlink:type="simple"/></inline-formula> at the observed data point<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-1240445x61.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-1240445x62.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-1240445x63.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-1240445x64.png" xlink:type="simple"/></inline-formula>. The signed log-likelihood ratio statistic r is</p><disp-formula id="scirp.54078-formula2457"><label>(9)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/7-1240445x65.png"  xlink:type="simple"/></disp-formula><p>and the standardized maximum likelihood departure <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-1240445x66.png" xlink:type="simple"/></inline-formula> re-calibrated in the <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-1240445x66.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-1240445x67.png" xlink:type="simple"/></inline-formula> scale is</p><disp-formula id="scirp.54078-formula2458"><graphic  xlink:href="http://html.scirp.org/file/7-1240445x68.png"  xlink:type="simple"/></disp-formula><p>Since<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-1240445x69.png" xlink:type="simple"/></inline-formula>, by applying the chain rule in differentiation, we have</p><disp-formula id="scirp.54078-formula2459"><graphic  xlink:href="http://html.scirp.org/file/7-1240445x70.png"  xlink:type="simple"/></disp-formula><p>where<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-1240445x71.png" xlink:type="simple"/></inline-formula>. Therefore, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-1240445x71.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-1240445x72.png" xlink:type="simple"/></inline-formula>can be written as</p><disp-formula id="scirp.54078-formula2460"><label>(10)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/7-1240445x73.png"  xlink:type="simple"/></disp-formula><p>Applications of the general method discussed above can be found is Reid and Fraser [<xref ref-type="bibr" rid="scirp.54078-ref10">10</xref>] and Davison et al. [<xref ref-type="bibr" rid="scirp.54078-ref11">11</xref>] .</p><p>Note that <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-1240445x74.png" xlink:type="simple"/></inline-formula> in (7) can be viewed as the sensitivity direction and is examined in Fraser et al. [<xref ref-type="bibr" rid="scirp.54078-ref12">12</xref>] for the</p><p>study of the sensitivity analysis of the third-order method. And <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-1240445x75.png" xlink:type="simple"/></inline-formula> gives the rate of change of the score</p><p>variable with respect to the change of <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-1240445x76.png" xlink:type="simple"/></inline-formula> at the observed data point in the tangent exponential model.</p></sec><sec id="s3"><title>3. Relationship between the Score Variable and the Locally Defined Canonical Parameter</title><p>In Bayesian analysis, Jeffreys [<xref ref-type="bibr" rid="scirp.54078-ref13">13</xref>] proposed to use the prior density which is proportional to the square root of the Fisher’s expected information. This prior is invariant under reparameterization. In other words, the scalar parameter</p><disp-formula id="scirp.54078-formula2461"><graphic  xlink:href="http://html.scirp.org/file/7-1240445x77.png"  xlink:type="simple"/></disp-formula><p>yields an information function <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-1240445x78.png" xlink:type="simple"/></inline-formula> that is constant in value. Since Fisher’s expected information</p><p>might be difficult to obtain, we can approximate it by the observed information evaluated at the maximum like- lihood estimate <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-1240445x79.png" xlink:type="simple"/></inline-formula> which is</p><disp-formula id="scirp.54078-formula2462"><graphic  xlink:href="http://html.scirp.org/file/7-1240445x80.png"  xlink:type="simple"/></disp-formula><p>Hence, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-1240445x81.png" xlink:type="simple"/></inline-formula>is approximately invariant under reparameterization.</p><p>Fraser et al. [<xref ref-type="bibr" rid="scirp.54078-ref12">12</xref>] showed that</p><disp-formula id="scirp.54078-formula2463"><label>(11)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/7-1240445x82.png"  xlink:type="simple"/></disp-formula><p>is a pivotal quantity to the second-order. A change of variable from the maximum likelihood estimate of locally defined canonical parameter <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-1240445x83.png" xlink:type="simple"/></inline-formula> to the score variable <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-1240445x83.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-1240445x84.png" xlink:type="simple"/></inline-formula> for the first integral of (11) yields</p><disp-formula id="scirp.54078-formula2464"><label>(12)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/7-1240445x85.png"  xlink:type="simple"/></disp-formula><p>which relates the score varaible to the locally defined canonical parameter. Taking the total derivative of (12), and evaluate at the observed data point, we have</p><disp-formula id="scirp.54078-formula2465"><graphic  xlink:href="http://html.scirp.org/file/7-1240445x86.png"  xlink:type="simple"/></disp-formula><p>Moreover, at<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-1240445x87.png" xlink:type="simple"/></inline-formula>,</p><disp-formula id="scirp.54078-formula2466"><graphic  xlink:href="http://html.scirp.org/file/7-1240445x88.png"  xlink:type="simple"/></disp-formula><p>Therefore, the rate of change of the score variable with respect to the change of the locally defined canonical parameter at the observed data point is</p><disp-formula id="scirp.54078-formula2467"><label>(13)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/7-1240445x89.png"  xlink:type="simple"/></disp-formula><p>This describes how the locally defined canonical parameter <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-1240445x90.png" xlink:type="simple"/></inline-formula> moves the score variable<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-1240445x90.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-1240445x91.png" xlink:type="simple"/></inline-formula>.</p></sec><sec id="s4"><title>4. Combining Likelihood Information</title><p>Assume we have <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-1240445x92.png" xlink:type="simple"/></inline-formula> independent investigations, each of them is used to obtain inference concerning a scalar parameter<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-1240445x92.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-1240445x93.png" xlink:type="simple"/></inline-formula>. Denote the log-likelihood function for the <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-1240445x92.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-1240445x93.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-1240445x94.png" xlink:type="simple"/></inline-formula> investigation be <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-1240445x92.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-1240445x93.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-1240445x94.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-1240445x95.png" xlink:type="simple"/></inline-formula> and the corresponding canonical parameter is<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-1240445x92.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-1240445x93.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-1240445x94.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-1240445x95.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-1240445x96.png" xlink:type="simple"/></inline-formula>. Note that if <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-1240445x92.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-1240445x93.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-1240445x94.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-1240445x95.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-1240445x96.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-1240445x97.png" xlink:type="simple"/></inline-formula> is not explicitly available, we can use the locally defined canonical variable as obtain from (9). The combined log-likelihood function is</p><disp-formula id="scirp.54078-formula2468"><graphic  xlink:href="http://html.scirp.org/file/7-1240445x98.png"  xlink:type="simple"/></disp-formula><p>and hence the maximum likelihood estimate of <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-1240445x99.png" xlink:type="simple"/></inline-formula> can be obtained. Therefore, the signed log-likelihood func- tion <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-1240445x99.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-1240445x100.png" xlink:type="simple"/></inline-formula> can be calculated from (12).</p><p>From (13), the rate of change of the score variable from the <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-1240445x101.png" xlink:type="simple"/></inline-formula> investigation with respect to the corre- sponding canonical paramter at the observed data from the <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-1240445x101.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-1240445x102.png" xlink:type="simple"/></inline-formula> investigation is</p><disp-formula id="scirp.54078-formula2469"><label>(14)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/7-1240445x103.png"  xlink:type="simple"/></disp-formula><p>where</p><disp-formula id="scirp.54078-formula2470"><graphic  xlink:href="http://html.scirp.org/file/7-1240445x104.png"  xlink:type="simple"/></disp-formula><p>Hence, the combined canonical parameter is</p><disp-formula id="scirp.54078-formula2471"><label>(15)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/7-1240445x105.png"  xlink:type="simple"/></disp-formula><p>The standardized maximum likelihood departure based on the combined canonical parameter can be cal- culated from (5). Thus, a new p-value can be obtained from the combined log-likelihood function and the com- bined canonical parameter using the Lugannani and Rice formula or the Barndorff-Nielsen formula.</p></sec><sec id="s5"><title>5. Examples</title><p>In this section, we first revisit the rate of arrival problem discussed in Section 1 and show that the proposed method gives results that is quite different from the results obtained by the Fisher’s way of combining p-values. Then simulation studies are performed to compare the accuracy of the proposed method with the Fisher’s method for the rate of arrival problem. Moreover, two well-known models: scalar canonical exponential family model and normal mean model, are examined. It is shown that, theoretically, the proposed method gives the same results as obtained by the third-order method that was discussed in Fraser and Reid [<xref ref-type="bibr" rid="scirp.54078-ref5">5</xref>] and DiCiccio et al. [<xref ref-type="bibr" rid="scirp.54078-ref14">14</xref>] , respectively.</p><sec id="s5_1"><title>5.1. Revisit the Rate of Arrival Problem</title><p>From the first investigation discussed in Section 1, the log-likelihood function for the Poisson model is</p><disp-formula id="scirp.54078-formula2472"><graphic  xlink:href="http://html.scirp.org/file/7-1240445x106.png"  xlink:type="simple"/></disp-formula><p>where <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-1240445x107.png" xlink:type="simple"/></inline-formula> is the canonical parameter. We have</p><disp-formula id="scirp.54078-formula2473"><graphic  xlink:href="http://html.scirp.org/file/7-1240445x108.png"  xlink:type="simple"/></disp-formula><p>Moreover, from the second investigation discussed in Section 1, the log-likelihood function for the exponen- tial model is</p><disp-formula id="scirp.54078-formula2474"><graphic  xlink:href="http://html.scirp.org/file/7-1240445x109.png"  xlink:type="simple"/></disp-formula><p>where <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-1240445x110.png" xlink:type="simple"/></inline-formula> is the canonical parameter. We have</p><disp-formula id="scirp.54078-formula2475"><graphic  xlink:href="http://html.scirp.org/file/7-1240445x111.png"  xlink:type="simple"/></disp-formula><p>The combined log-likelihood function is</p><disp-formula id="scirp.54078-formula2476"><graphic  xlink:href="http://html.scirp.org/file/7-1240445x112.png"  xlink:type="simple"/></disp-formula><p>and we have</p><disp-formula id="scirp.54078-formula2477"><graphic  xlink:href="http://html.scirp.org/file/7-1240445x113.png"  xlink:type="simple"/></disp-formula><p>Therefore,</p><disp-formula id="scirp.54078-formula2478"><graphic  xlink:href="http://html.scirp.org/file/7-1240445x114.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.54078-formula2479"><graphic  xlink:href="http://html.scirp.org/file/7-1240445x115.png"  xlink:type="simple"/></disp-formula><p>and from (17) we have <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-1240445x116.png" xlink:type="simple"/></inline-formula> and<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-1240445x116.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-1240445x117.png" xlink:type="simple"/></inline-formula>. Thus, the combined locally defined canonical para- meter is</p><disp-formula id="scirp.54078-formula2480"><graphic  xlink:href="http://html.scirp.org/file/7-1240445x118.png"  xlink:type="simple"/></disp-formula><p>Hence, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-1240445x119.png" xlink:type="simple"/></inline-formula>is obtained from (12) using the combined log-likelihood function. Since the signed log- likelihood ration statistic is asymptotically distributed as a standard normal distribution, the p-value obtained from the signed log-likelihood ratio method is 0.0565. It is well-known that the signed log-likelihood ratio method has only first order accuracy. From (8) using the combined locally defined canonical parameter, we have<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-1240445x119.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-1240445x120.png" xlink:type="simple"/></inline-formula>. Finally, the p-value obtained by the Lugannani and Rice formula and by the Barndorff-Nielsen formula is 0.0600, which is less certain about the evidence that <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-1240445x119.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-1240445x120.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-1240445x121.png" xlink:type="simple"/></inline-formula> is greater than 1 as suggested by the result from Fisher’s way of combining of p-values. Note that in literature, there are many detailed studies comparing the accuracy of the first order and third order methods (see Barndorff-Nielsen [<xref ref-type="bibr" rid="scirp.54078-ref4">4</xref>] , Fraser [<xref ref-type="bibr" rid="scirp.54078-ref6">6</xref>] , Jensen [<xref ref-type="bibr" rid="scirp.54078-ref7">7</xref>] , Brazzale et al. [<xref ref-type="bibr" rid="scirp.54078-ref8">8</xref>] , and DiCiccio et al. [<xref ref-type="bibr" rid="scirp.54078-ref14">14</xref>] ). Thus, in this paper, we will not compare the signed log-likelihood ratio method and the proposed method.</p><p><xref ref-type="fig" rid="fig1">Figure 1</xref> plot <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-1240445x122.png" xlink:type="simple"/></inline-formula> obtained from Fisher’s method, Lugannani and Rice method and Barndorff- Nielsen method. From the plot, it is clear that the two proposed methods give almost identical results, which are very different from the results obtained by the Fisher’s method.</p></sec><sec id="s5_2"><title>5.2. Simulation Study</title><p>Simulation studies are performed to compare the three methods discussed in this paper. We examine the rate of arrival problem that was discussed in Section 1. For each combination of<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-1240445x123.png" xlink:type="simple"/></inline-formula>, we</p><p>1) generate <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-1240445x124.png" xlink:type="simple"/></inline-formula> from Poisson<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-1240445x124.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-1240445x125.png" xlink:type="simple"/></inline-formula>, and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-1240445x124.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-1240445x125.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-1240445x126.png" xlink:type="simple"/></inline-formula> from exponential <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-1240445x124.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-1240445x125.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-1240445x126.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-1240445x127.png" xlink:type="simple"/></inline-formula></p><p>2) calculate p-values obtained by the three methods discussed in this paper;</p><fig id="fig1"  position="float"><label><xref ref-type="fig" rid="fig1">Figure 1</xref></label><caption><title> p-value function</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/7-1240445x128.png"/></fig><p>3) record if the p-value is less than a preset value <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-1240445x129.png" xlink:type="simple"/></inline-formula></p><p>4) repeat this process <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-1240445x130.png" xlink:type="simple"/></inline-formula> times.</p><p>Finally, report the proportion of p-values that is less than <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-1240445x131.png" xlink:type="simple"/></inline-formula> and this value, sometimes, is referred to as the simulated Type I errors. For an accurate method, the result should be close to<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-1240445x131.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-1240445x132.png" xlink:type="simple"/></inline-formula>. The simulated standard error</p><p>of this process is<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-1240445x133.png" xlink:type="simple"/></inline-formula>.</p><p><xref ref-type="table" rid="table1">Table 1</xref> recorded the simulated Type I errors obtained by the Fisher’s method (Fisher), Lugannani and Rice method (LR) and Barndorff-Nielsen method (BN). Results from <xref ref-type="table" rid="table1">Table 1</xref> illustrated that the proposed methods are extremely accurate as they are all within 3 simulated standard errors. And the results by the Fisher’s method are not satisfactory as they are way larger than the prescriped <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-1240445x134.png" xlink:type="simple"/></inline-formula> values.</p></sec><sec id="s5_3"><title>5.3. Scalar Canonical Exponential Family Model</title><p>Consider <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-1240445x135.png" xlink:type="simple"/></inline-formula> independent investigations from canonical exponential family model with density</p><disp-formula id="scirp.54078-formula2481"><graphic  xlink:href="http://html.scirp.org/file/7-1240445x136.png"  xlink:type="simple"/></disp-formula><p>where <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-1240445x137.png" xlink:type="simple"/></inline-formula> is the scalar canonical parameter of interest and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-1240445x137.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-1240445x138.png" xlink:type="simple"/></inline-formula> is the minimal sufficient statistic for the <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-1240445x137.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-1240445x138.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-1240445x139.png" xlink:type="simple"/></inline-formula> model.</p><p>From the above model, we have<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-1240445x140.png" xlink:type="simple"/></inline-formula>. The log-likelihood function and its corresponding deri- vatives are</p><disp-formula id="scirp.54078-formula2482"><graphic  xlink:href="http://html.scirp.org/file/7-1240445x141.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.54078-formula2483"><graphic  xlink:href="http://html.scirp.org/file/7-1240445x142.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.54078-formula2484"><graphic  xlink:href="http://html.scirp.org/file/7-1240445x143.png"  xlink:type="simple"/></disp-formula><p>where<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-1240445x144.png" xlink:type="simple"/></inline-formula>. Hence <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-1240445x144.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-1240445x145.png" xlink:type="simple"/></inline-formula> has to satisfy<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-1240445x144.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-1240445x145.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-1240445x146.png" xlink:type="simple"/></inline-formula>, and the observed information evaluated at</p><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-1240445x147.png" xlink:type="simple"/></inline-formula>is<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-1240445x147.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-1240445x148.png" xlink:type="simple"/></inline-formula>. The combined log-likelihood function is</p><disp-formula id="scirp.54078-formula2485"><graphic  xlink:href="http://html.scirp.org/file/7-1240445x149.png"  xlink:type="simple"/></disp-formula><table-wrap id="table1" ><label><xref ref-type="table" rid="table1">Table 1</xref></label><caption><title> Simulated Type I errors (based on 10,000 simulated sample)</title></caption><table><tbody><thead><tr><th align="center" valign="middle" ></th><th align="center" valign="middle" ></th><th align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-1240445x150.png" xlink:type="simple"/></inline-formula></th><th align="center" valign="middle" ></th><th align="center" valign="middle" ></th><th align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-1240445x151.png" xlink:type="simple"/></inline-formula></th><th align="center" valign="middle" ></th><th align="center" valign="middle" ></th><th align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-1240445x152.png" xlink:type="simple"/></inline-formula></th><th align="center" valign="middle" ></th><th align="center" valign="middle" ></th></tr></thead><tr><td align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-1240445x153.png" xlink:type="simple"/></inline-formula></td><td align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-1240445x154.png" xlink:type="simple"/></inline-formula></td><td align="center" valign="middle" >Fisher</td><td align="center" valign="middle" >LR</td><td align="center" valign="middle" >BN</td><td align="center" valign="middle" >Fisher</td><td align="center" valign="middle" >LR</td><td align="center" valign="middle" >BN</td><td align="center" valign="middle" >Fisher</td><td align="center" valign="middle" >LR</td><td align="center" valign="middle" >BN</td></tr><tr><td align="center" valign="middle" >5</td><td align="center" valign="middle" >0.1</td><td align="center" valign="middle" >0.2459</td><td align="center" valign="middle" >0.1084</td><td align="center" valign="middle" >0.1073</td><td align="center" valign="middle" >0.1231</td><td align="center" valign="middle" >0.0525</td><td align="center" valign="middle" >0.0521</td><td align="center" valign="middle" >0.0225</td><td align="center" valign="middle" >0.0099</td><td align="center" valign="middle" >0.0097</td></tr><tr><td align="center" valign="middle" ></td><td align="center" valign="middle" >1.0</td><td align="center" valign="middle" >0.3252</td><td align="center" valign="middle" >0.0992</td><td align="center" valign="middle" >0.0992</td><td align="center" valign="middle" >0.1908</td><td align="center" valign="middle" >0.0496</td><td align="center" valign="middle" >0.0496</td><td align="center" valign="middle" >0.0515</td><td align="center" valign="middle" >0.0123</td><td align="center" valign="middle" >0.0123</td></tr><tr><td align="center" valign="middle" ></td><td align="center" valign="middle" >2.0</td><td align="center" valign="middle" >0.3256</td><td align="center" valign="middle" >0.1025</td><td align="center" valign="middle" >0.1025</td><td align="center" valign="middle" >0.1961</td><td align="center" valign="middle" >0.0513</td><td align="center" valign="middle" >0.0513</td><td align="center" valign="middle" >0.0547</td><td align="center" valign="middle" >0.0112</td><td align="center" valign="middle" >0.0112</td></tr><tr><td align="center" valign="middle" >10</td><td align="center" valign="middle" >0.5</td><td align="center" valign="middle" >0.3318</td><td align="center" valign="middle" >0.1014</td><td align="center" valign="middle" >0.1014</td><td align="center" valign="middle" >0.1942</td><td align="center" valign="middle" >0.0490</td><td align="center" valign="middle" >0.0490</td><td align="center" valign="middle" >0.0513</td><td align="center" valign="middle" >0.0128</td><td align="center" valign="middle" >0.0128</td></tr><tr><td align="center" valign="middle" ></td><td align="center" valign="middle" >1.0</td><td align="center" valign="middle" >0.3325</td><td align="center" valign="middle" >0.1005</td><td align="center" valign="middle" >0.1005</td><td align="center" valign="middle" >0.1965</td><td align="center" valign="middle" >0.0530</td><td align="center" valign="middle" >0.0530</td><td align="center" valign="middle" >0.0574</td><td align="center" valign="middle" >0.0105</td><td align="center" valign="middle" >0.0105</td></tr><tr><td align="center" valign="middle" ></td><td align="center" valign="middle" >2.0</td><td align="center" valign="middle" >0.3269</td><td align="center" valign="middle" >0.1006</td><td align="center" valign="middle" >0.1006</td><td align="center" valign="middle" >0.1975</td><td align="center" valign="middle" >0.0513</td><td align="center" valign="middle" >0.0513</td><td align="center" valign="middle" >0.0562</td><td align="center" valign="middle" >0.0107</td><td align="center" valign="middle" >0.0107</td></tr><tr><td align="center" valign="middle" >20</td><td align="center" valign="middle" >1.0</td><td align="center" valign="middle" >0.3365</td><td align="center" valign="middle" >0.1000</td><td align="center" valign="middle" >0.1000</td><td align="center" valign="middle" >0.2018</td><td align="center" valign="middle" >0.0526</td><td align="center" valign="middle" >0.0526</td><td align="center" valign="middle" >0.0546</td><td align="center" valign="middle" >0.0098</td><td align="center" valign="middle" >0.0096</td></tr><tr><td align="center" valign="middle" ></td><td align="center" valign="middle" >2.0</td><td align="center" valign="middle" >0.3387</td><td align="center" valign="middle" >0.1064</td><td align="center" valign="middle" >0.1064</td><td align="center" valign="middle" >0.2027</td><td align="center" valign="middle" >0.0528</td><td align="center" valign="middle" >0.0528</td><td align="center" valign="middle" >0.0578</td><td align="center" valign="middle" >0.0109</td><td align="center" valign="middle" >0.0109</td></tr><tr><td align="center" valign="middle" ></td><td align="center" valign="middle" >5.0</td><td align="center" valign="middle" >0.3356</td><td align="center" valign="middle" >0.1048</td><td align="center" valign="middle" >0.1048</td><td align="center" valign="middle" >0.2037</td><td align="center" valign="middle" >0.0528</td><td align="center" valign="middle" >0.0528</td><td align="center" valign="middle" >0.0582</td><td align="center" valign="middle" >0.0111</td><td align="center" valign="middle" >0.0111</td></tr></tbody></table></table-wrap><p>and the log-likelihood ratio statistic obtained from the combined log-likelihood function can be obtained from (12). Moreover, from (17), we have</p><disp-formula id="scirp.54078-formula2486"><graphic  xlink:href="http://html.scirp.org/file/7-1240445x155.png"  xlink:type="simple"/></disp-formula><p>and hence the combined canonical parameter is</p><disp-formula id="scirp.54078-formula2487"><graphic  xlink:href="http://html.scirp.org/file/7-1240445x156.png"  xlink:type="simple"/></disp-formula><p>The maximum likelihood departure in the combined canonical parameter space is</p><disp-formula id="scirp.54078-formula2488"><graphic  xlink:href="http://html.scirp.org/file/7-1240445x157.png"  xlink:type="simple"/></disp-formula><p>with the observed information evaluated at <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-1240445x158.png" xlink:type="simple"/></inline-formula> being</p><disp-formula id="scirp.54078-formula2489"><graphic  xlink:href="http://html.scirp.org/file/7-1240445x159.png"  xlink:type="simple"/></disp-formula><p>and thus,</p><disp-formula id="scirp.54078-formula2490"><graphic  xlink:href="http://html.scirp.org/file/7-1240445x160.png"  xlink:type="simple"/></disp-formula><p>which is the same as directly applying the third-order method to the canonical exponential family model with <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-1240445x161.png" xlink:type="simple"/></inline-formula> being the canoncial parameter as discussed in Fraser and Reid [<xref ref-type="bibr" rid="scirp.54078-ref5">5</xref>] .</p></sec><sec id="s5_4"><title>5.4. Normal Mean Model</title><p>Consider <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-1240445x162.png" xlink:type="simple"/></inline-formula> independent investigations from normal mean model with density</p><disp-formula id="scirp.54078-formula2491"><graphic  xlink:href="http://html.scirp.org/file/7-1240445x163.png"  xlink:type="simple"/></disp-formula><p>where <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-1240445x164.png" xlink:type="simple"/></inline-formula> is the mean parameter of interest. The pivotal quantity is<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-1240445x164.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-1240445x165.png" xlink:type="simple"/></inline-formula>. Hence, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-1240445x164.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-1240445x165.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-1240445x166.png" xlink:type="simple"/></inline-formula>, and</p><disp-formula id="scirp.54078-formula2492"><graphic  xlink:href="http://html.scirp.org/file/7-1240445x167.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.54078-formula2493"><graphic  xlink:href="http://html.scirp.org/file/7-1240445x168.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.54078-formula2494"><graphic  xlink:href="http://html.scirp.org/file/7-1240445x169.png"  xlink:type="simple"/></disp-formula><p>with <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-1240445x170.png" xlink:type="simple"/></inline-formula> and<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-1240445x170.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-1240445x171.png" xlink:type="simple"/></inline-formula>. The combined log-likelihood function is</p><disp-formula id="scirp.54078-formula2495"><graphic  xlink:href="http://html.scirp.org/file/7-1240445x172.png"  xlink:type="simple"/></disp-formula><p>with <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-1240445x173.png" xlink:type="simple"/></inline-formula> and<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-1240445x173.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-1240445x174.png" xlink:type="simple"/></inline-formula>. From (17), we have <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-1240445x173.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-1240445x174.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-1240445x175.png" xlink:type="simple"/></inline-formula> and, therefore the combined canonical parameter is</p><disp-formula id="scirp.54078-formula2496"><graphic  xlink:href="http://html.scirp.org/file/7-1240445x176.png"  xlink:type="simple"/></disp-formula><p>and<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-1240445x177.png" xlink:type="simple"/></inline-formula>. Finally, from Equation (12), the signed log-likelihood ratio statistic is</p><disp-formula id="scirp.54078-formula2497"><graphic  xlink:href="http://html.scirp.org/file/7-1240445x178.png"  xlink:type="simple"/></disp-formula><p>and the standardized maximum likelihood departure calculated in the locally defined canonical parameter scale can be obtained from Equation (8) and is</p><disp-formula id="scirp.54078-formula2498"><graphic  xlink:href="http://html.scirp.org/file/7-1240445x179.png"  xlink:type="simple"/></disp-formula><p>These are exactly the same as those obtained in DiCiccio et al. [<xref ref-type="bibr" rid="scirp.54078-ref14">14</xref>] .</p></sec></sec><sec id="s6"><title>6. Conclusion</title><p>In this paper, a method is proposed to obtain a p-value by combining the likelihood functions and the standardized maximum likelihood estimates departure calculated in the canonical parameter space of independent investigations for testing a scalar parameter of interest. It is shown that for the canonical exponential model and the normal mean model, the proposed method gives exactly the same results as using the joint likelihood function. Moreover, for the rate of arrival problem, the proposed method gives very different results from the results obtained by the Fisher’s way of combining p-values. And simulation studies illustrate that the proposed method is extremely accurate.</p></sec><sec id="s7"><title>Acknowledgements</title><p>This research was supported in part by and the National Sciences and Engineering Research Council of Canada.</p></sec></body><back><ref-list><title>References</title><ref id="scirp.54078-ref1"><label>1</label><mixed-citation publication-type="other" xlink:type="simple">Fisher, R.A. (1925) Statistical Methods for Research Workers. Oliver and Boyd, Edinburg.</mixed-citation></ref><ref id="scirp.54078-ref2"><label>2</label><mixed-citation publication-type="other" xlink:type="simple">Lugannani, R. and Rice, S. 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