<?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">TEL</journal-id><journal-title-group><journal-title>Theoretical Economics Letters</journal-title></journal-title-group><issn pub-type="epub">2162-2078</issn><publisher><publisher-name>Scientific Research Publishing</publisher-name></publisher></journal-meta><article-meta><article-id pub-id-type="doi">10.4236/tel.2012.22034</article-id><article-id pub-id-type="publisher-id">TEL-19296</article-id><article-categories><subj-group subj-group-type="heading"><subject>Articles</subject></subj-group><subj-group subj-group-type="Discipline-v2"><subject>Business&amp;Economics</subject></subj-group></article-categories><title-group><article-title>
 
 
  Hyperbolic Transformation and Average Elasticity in the Framework of the Fixed Effects Logit Model
 
</article-title></title-group><contrib-group><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>oshitsugu</surname><given-names>Kitazawa</given-names></name><xref ref-type="aff" rid="aff1"><sub>1</sub></xref><xref ref-type="corresp" rid="cor1"><sup>*</sup></xref></contrib></contrib-group><aff id="aff1"><label>1</label><addr-line>Faculty of Economics, Kyushu Sangyo University, Fukuoka, Japan</addr-line></aff><author-notes><corresp id="cor1">* E-mail:<email>kitazawa@ip.kyusan-u.ac.jp</email></corresp></author-notes><pub-date pub-type="epub"><day>23</day><month>05</month><year>2012</year></pub-date><volume>02</volume><issue>02</issue><fpage>192</fpage><lpage>199</lpage><history><date date-type="received"><day>January</day>	<month>13,</month>	<year>2012</year></date><date date-type="rev-recd"><day>February</day>	<month>11,</month>	<year>2012</year>	</date><date date-type="accepted"><day>February</day>	<month>20,</month>	<year>2012</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>
 
 
  In this paper, a simple transformation is proposed for the fixed effects logit model, which constructs some valid moment conditions including the first-order condition for one of the conditional MLE proposed by Chamberlain (1980) [1]. Some Monte Carlo experiments are carried out for the GMM estimator based on the transformation. In addition, the average elasticity of the logit probability with respect to the exponential function of explanatory variable is proposed in the framework of the fixed effects logit model, which is computable without the fixed effects.
 
</p></abstract><kwd-group><kwd>Fixed Effects Logit; Conditional Logit Estimator; Hyperbolic Transformation; Moment Conditions; GMM; Monte Carlo Experiments; Average Elasticity</kwd></kwd-group></article-meta></front><body><sec id="s1"><title>1. Introduction</title><p>Chamberlain (1980) [<xref ref-type="bibr" rid="scirp.19296-ref1">1</xref>] proposes the useful and established estimator for the fixed effects logit model in panel data.1 This estimator is referred to as the conditional logit estimator, which maximizes the likelihood function composed of the probabilities of the (binary) dependent variables conditional on the fixed effects, the (real-valued) explanatory variables, and the intertemporal sums of the dependent variables. The conditional logit estimator is consistent for the situation of small number of time periods and large cross-sectional size, since its conditional likelihood function rules out the fixed effects and accordingly circumvents the incidental parameters problems pointed out by Neyman and Scott (1948) [<xref ref-type="bibr" rid="scirp.19296-ref2">2</xref>].2 This paper advocates another method of consistently estimating the fixed effects logit model for the situation of small number of time periods and large cross-sectional size.3 The procedure of the method is as follows: First, a hyperbolic transformation is applied to the fixed effects logit model with the aim of eliminating the fixed effects. Next, the GMM (generalized method of moments) estimator proposed by Hansen (1982) [<xref ref-type="bibr" rid="scirp.19296-ref20">20</xref>] is constructed by using the moment conditions based on the hyperbolic transformation. It will be seen that these moment conditions include one type of the first-order conditions of the likelihood for the conditional logit estimator. Then, the preferable small sample property of the GMM estimator using the moment conditions based on the hyperbolic transformation is shown by some Monte Carlo experiments.</p><p>In addition, this paper presents the calculation formula of the average elasticity of the logit probability with respect to the exponential function of explanatory variable for the fixed effects logit model. The average marginal effect is not obtained due to the incidental parameters problems for the case of the fixed effects logit model with time dimension being strictly fixed, while it seems that no appropriate index measuring the effect of the change of explanatory variable is developed, in author’s best knowledge. Since the average elasticity is able to be calculated using the consistent estimator of the parameter of interest and the average of binary dependent variables without relation to the fixed effects, it can be said that it is a revolutionary index for the fixed effects logit model.</p><p>The rest of the paper is as follows: Section 2 presents the implicit form of the fixed effects logit model, the moment conditions based on the hyperbolic transformation, and the GMM estimator. Section 3 illustrates the link between the conditional maximum likelihood estimator (CMLE) mentioned in the first paragraph in this section and the GMM estimator for the case of two periods. Section 4 reports some Monte Carlo results for the GMM estimator. Section 5 presents the average elasticity in the framework of the fixed effects logit model. Section 6 concludes.</p></sec><sec id="s2"><title>2. Fixed Effects Logit Model, Hyperbolic Transformation and GMM Estimator</title><p>In this section, the (static) fixed effects logit model is implicitly defined where the error term is of additive form.4 The hyperbolic transformation, which eliminates the fixed effects and then based on which the moment conditions is constructed for estimating the model consistently, is the fruits of the model defined implicitly. The GMM estimator is defined by using the moment conditions constructed. Throughout this paper, the subscripts <img src="14-1500105\2f4f3614-9a46-4733-9968-0cb1af03264b.jpg" /> and <img src="14-1500105\2d04142c-f8ee-4a90-af42-5dc26637bf77.jpg" /> denote the individual and time period respectively, while <img src="14-1500105\80864df1-0519-4682-baf5-0933a8d8ea69.jpg" /> and <img src="14-1500105\bc251f67-690a-4d1f-9209-3849d92e1296.jpg" /> are number of individuals and number of time periods respectively. Since the short panel is supposed, it is assumed that <img src="14-1500105\fc8ee09b-c93d-42cb-b54b-fd6a20740bf9.jpg" /> and <img src="14-1500105\4e4406d4-89b1-4e01-ade0-afc5b663e057.jpg" /> is fixed. In addition, it is assumed that the variables in the model are independent among individuals.</p><p>The fixed effects logit model is able to be written in the implicit form as follows:</p><p><img src="14-1500105\9d2fe69a-3ef5-459e-b3db-505e9a040414.jpg" />, for<img src="14-1500105\0f8fd339-79a1-418b-8567-7d71e8a132ec.jpg" />,(2.1)</p><disp-formula id="scirp.19296-formula35259"><label>(2.2)</label><graphic position="anchor" xlink:href="14-1500105\0a8a489c-a561-4610-a29a-257d8d4fd040.jpg"  xlink:type="simple"/></disp-formula><p>where the observable variables <img src="14-1500105\f11b88bb-b082-4ab8-b311-4d09e3de5600.jpg" /> and <img src="14-1500105\4a262090-8c5d-4efa-846e-9ade88871d51.jpg" /> are the binary dependent variable and the real-valued explanatory variable respectively, while the unobservable variables <img src="14-1500105\4de7d782-92d3-4de0-9219-6571ad82ff02.jpg" /> and <img src="14-1500105\2d768b7c-4792-42c4-88ab-01a399d3a8ba.jpg" /> are the individual fixed effect and the disturbance respectively.5 Equations (2.1) say that <img src="14-1500105\287521ef-d06f-4f02-8851-67703d187edf.jpg" /> take one with probability<img src="14-1500105\42dfc609-9569-4f10-99bc-d1102e73b5c2.jpg" />, while it is seen from Equations (2.2) that the probability is the logistic cumulative distribution function of<img src="14-1500105\109b1fb5-63f5-4c4c-b01d-3f917e80c3fd.jpg" />. Allowing for the serially uncorrelated disturbances, the uncorrelatedness between the disturbances and the fixed effect and the strictly exogenous explanatory variables, the assumptions on the disturbances are specified as</p><p><img src="14-1500105\403917cb-c9e4-4c7f-85d9-d75b12ab5d16.jpg" />, for<img src="14-1500105\713501eb-63c4-49a1-b3aa-05c35e8def4d.jpg" />,(2.3)</p><p>where <img src="14-1500105\f015dd1b-7b6a-4cf1-acc9-948fcdf3caa5.jpg" /> for<img src="14-1500105\7620fc90-3988-4822-aa3c-162d8437d932.jpg" />, <img src="14-1500105\82dea8b0-c8f7-4b72-9e6c-54afdec63043.jpg" />is defined as the empty set for convenience and</p><p><img src="14-1500105\1d159219-42c8-4867-bcd0-445ee2f47403.jpg" />. The assumptions (2.3) can be derived from the assumption underlying the fixed effects logit model, which is that <img src="14-1500105\2b7922b4-20d9-4531-9bbb-ec80782af701.jpg" /> for <img src="14-1500105\be2653db-a7e3-4684-960b-c2ae44315eaa.jpg" /> are mutually independent conditional on <img src="14-1500105\ae44833c-285b-4c9f-8f0e-c7fbc6465733.jpg" /> and<img src="14-1500105\be367c6e-3996-4f84-8086-43ae6424e53e.jpg" />.6 From now on, based on the fixed effects logit model composed of (2.1) and (2.2) with (2.3), the moment conditions for estimating the parameter of interest <img src="14-1500105\814026ca-8e0f-4a3a-8514-c097e655dde1.jpg" /> consistently are constructed by using a hyperbolic transformation, as stated below. Taking notice of the fact that</p><disp-formula id="scirp.19296-formula35260"><label>(2.4)</label><graphic position="anchor" xlink:href="14-1500105\b0337b3c-df51-4c9b-b48d-4b68322ef032.jpg"  xlink:type="simple"/></disp-formula><p>and using the formula that</p><disp-formula id="scirp.19296-formula35261"><label>(2.5)</label><graphic position="anchor" xlink:href="14-1500105\0511ab8b-6870-4d93-b0b1-f16f9732c76a.jpg"  xlink:type="simple"/></disp-formula><p>with <img src="14-1500105\231f0556-2e86-41f9-afda-68f49b27dea9.jpg" /> and <img src="14-1500105\88623250-14d0-4b37-bbf4-59d7a1008c53.jpg" /> being any real numbers, it follows that</p><disp-formula id="scirp.19296-formula35262"><label>, (2.6)</label><graphic position="anchor" xlink:href="14-1500105\300e91a5-4f47-41a3-891a-cafcfd4a583c.jpg"  xlink:type="simple"/></disp-formula><p>where <img src="14-1500105\fc8598f9-130a-414d-876d-87ff38534299.jpg" /> is the first differencing operator, such as<img src="14-1500105\76d7fd70-bd5e-45ce-b03c-38908e4a0f7e.jpg" />. Since <img src="14-1500105\3780c2cb-cff9-4950-bc4c-575d279e8a31.jpg" /> and <img src="14-1500105\28e41775-a55f-4334-88e3-d111dfdb442d.jpg" /> are written as</p><disp-formula id="scirp.19296-formula35263"><label>(2.7)</label><graphic position="anchor" xlink:href="14-1500105\2f188c33-7ce9-4183-9fd9-3bfd45272384.jpg"  xlink:type="simple"/></disp-formula><p>and</p><disp-formula id="scirp.19296-formula35264"><label>(2.8)</label><graphic position="anchor" xlink:href="14-1500105\75c28aaf-a76d-4bb7-98c1-d5d533daae5c.jpg"  xlink:type="simple"/></disp-formula><p>respectively by using (2.1) and (2.3), plugging (2.7) and (2.8) into (2.6) gives</p><p><img src="14-1500105\162de9b9-ba10-4ce6-b9ca-31ee56c7dbea.jpg" />(2.9)</p><p>Equations (2.7) and (2.8) are obtained by plugging (2.1) into <img src="14-1500105\a0ebeef4-a9cb-423a-becb-fca7947a5053.jpg" /> and</p><p><img src="14-1500105\038d6877-d53a-4c9f-9e49-503828fe6eb5.jpg" />and then applying (2.3) to them.</p><p>Taking the expectation conditional on <img src="14-1500105\7a3197bf-a1d4-4372-8a94-94034a2e2cac.jpg" /> for both sides of (2.9) and then applying law of iterated expectation and (2.3) dated<img src="14-1500105\fdbe3f80-fba8-40bd-b67d-c75a7aaa7db4.jpg" />, it follows that</p><disp-formula id="scirp.19296-formula35265"><label>(2.10)</label><graphic position="anchor" xlink:href="14-1500105\b3f0f71f-82ef-4a71-a6bd-06aa9c47498d.jpg"  xlink:type="simple"/></disp-formula><p>Since <img src="14-1500105\ec9ccd1e-dae6-4605-92de-039e480e8f62.jpg" /> for any positive integer value <img src="14-1500105\f4a22e22-f6c5-4af0-8ae2-853fd26ae649.jpg" /> due to the property of binary variable (and accordingly <img src="14-1500105\e70f521c-9475-4bdc-9988-ce5f371937b6.jpg" /> and<img src="14-1500105\edcb3211-339b-4a3c-b500-f9258f784f6f.jpg" />), Equation (2.10) results in</p><p><img src="14-1500105\9657ccb3-4d1f-4953-a33f-b0a1a313880e.jpg" />, for<img src="14-1500105\92b97151-aa48-4018-9d45-b224a31ea7b8.jpg" />, (2.11)</p><p>where</p><disp-formula id="scirp.19296-formula35266"><label>. (2.12)</label><graphic position="anchor" xlink:href="14-1500105\f60c975d-13d3-4de9-b5f8-96749340d5bc.jpg"  xlink:type="simple"/></disp-formula><p>The transformation (2.12) is referred to as “the hyperbolic tangent differencing transformation” for the fixed effects logit model in this paper and hereafter abbreviated to “the HTD transformation”.7 It should be noted that as seen from (2.11) and (2.12), observations for which <img src="14-1500105\89abccd1-7831-40eb-87d2-fcecd57392f6.jpg" /> and <img src="14-1500105\8df483c3-3bae-4082-8e9f-925d8018cce0.jpg" /> make no direct contribution to obtaining the estimates of <img src="14-1500105\89ae3468-097f-4bec-986c-9780597fa098.jpg" /> based on the moment conditions (2.11), since <img src="14-1500105\b038b2ee-7374-4b4d-bc57-db23426fc05e.jpg" /> is invariably zero for these observations.</p><p>The conditional moment conditions (2.11) give the following <img src="14-1500105\cbdbcb38-743e-4a7c-a92f-33c600a9de9e.jpg" /> vector of unconditional moment conditions:</p><disp-formula id="scirp.19296-formula35267"><label>, (2.13)</label><graphic position="anchor" xlink:href="14-1500105\cc6a933a-9fd0-4b6e-8b80-8bc34f61c6b6.jpg"  xlink:type="simple"/></disp-formula><p>where <img src="14-1500105\e19b4e98-fc26-4e0c-82e5-f5b41320660d.jpg" /> is the <img src="14-1500105\a4bd7eaf-e6ac-4c31-84ec-252ef086b939.jpg" /> vector and <img src="14-1500105\1b625bb8-d7d1-4e5a-a58f-9694b35032c4.jpg" /> is the <img src="14-1500105\b912cf22-f9d5-416d-aafc-bd95072c31cd.jpg" /> matrix with<img src="14-1500105\62f5949a-532c-4a64-87b5-d551426eb998.jpg" />. The (transposed) blocks</p><p><img src="14-1500105\8a5fc168-e7ec-4c97-a974-82e8b1eb1eb9.jpg" />, for<img src="14-1500105\72f492e7-0044-48da-a2c2-e6ebc6a89919.jpg" />, (2.14)</p><p>are the <img src="14-1500105\b1581311-434d-4c1f-ae7d-91b6a7a65933.jpg" /> vector-valued functions of<img src="14-1500105\197110d5-4704-4e44-9611-a326df55161f.jpg" />, <img src="14-1500105\53a5215b-aaaf-46a2-9846-560c41996344.jpg" />and <img src="14-1500105\e1fde8c4-2daa-44b9-8be3-4c7507346f82.jpg" /> at time<img src="14-1500105\b2f9b2a4-7706-48a4-98ad-cf0450035198.jpg" />, where <img src="14-1500105\35dd168f-7045-42e2-a3df-77b104051512.jpg" /> is number of instruments for time<img src="14-1500105\876ae487-f353-4529-96cb-8af48c85b369.jpg" />. By using the empirical counterpart of (2.13):</p><disp-formula id="scirp.19296-formula35268"><label>(2.15)</label><graphic position="anchor" xlink:href="14-1500105\00c7baa7-7f10-4534-b552-600d0605047d.jpg"  xlink:type="simple"/></disp-formula><p>and the <img src="14-1500105\0941f26f-122b-48b1-bbfe-e27da7bd98df.jpg" /> inverse of optimal weighting matrix:</p><disp-formula id="scirp.19296-formula35269"><label>, (2.16)</label><graphic position="anchor" xlink:href="14-1500105\6b966db9-a03b-4532-ae61-8a5582b235c9.jpg"  xlink:type="simple"/></disp-formula><p>where <img src="14-1500105\402c08ba-8c60-4d01-a2d0-235de446c172.jpg" /> is any initial consistent estimator for<img src="14-1500105\39965a58-9879-4b7a-a660-0618ee80cca6.jpg" />, the GMM estimator is constructed as follows:</p><disp-formula id="scirp.19296-formula35270"><label>, (2.17)</label><graphic position="anchor" xlink:href="14-1500105\eb48f9eb-bb6e-42f0-8a2c-7d6d22cdc722.jpg"  xlink:type="simple"/></disp-formula><p>where <img src="14-1500105\773dd2e7-ee61-4a43-8c1f-4ca4f52c13c8.jpg" /> converges in distribution to the normal distribution as follows:</p><disp-formula id="scirp.19296-formula35271"><label>(2.18)</label><graphic position="anchor" xlink:href="14-1500105\531eb9b1-8766-443f-8611-37b72233057b.jpg"  xlink:type="simple"/></disp-formula><p>with <img src="14-1500105\d9043861-7482-4d56-be65-97e661d74763.jpg" /> being the true value of<img src="14-1500105\634d4eea-0d77-4679-a9b0-d60cad751c94.jpg" />. Taking notice of the assumption that the variables are independent among individuals and adding the assumption that the variables are identically distributed among individuals, <img src="14-1500105\b8c571ff-6d4f-4f3e-b98a-310df7b90901.jpg" />, which is the (asymptotic) variance-covariance matrix of the moment conditions (2.13), can be written by using <img src="14-1500105\aececc87-7c60-4533-a947-29f389814e38.jpg" /> as follows:</p><disp-formula id="scirp.19296-formula35272"><label>, (2.19)</label><graphic position="anchor" xlink:href="14-1500105\acff301c-e8a1-4b48-98cc-43d820d290ab.jpg"  xlink:type="simple"/></disp-formula><p>where it should be noted that (2.16) is the empirical counterpart of (2.19) if <img src="14-1500105\0f355266-053f-472c-aec5-ec7e40820c5b.jpg" /> is replaced by <img src="14-1500105\a1d142ae-e556-41bf-8b5b-3681800d5883.jpg" /> and</p><p><img src="14-1500105\9c628b44-1e18-436d-b58a-a81490d942fb.jpg" />. Further, the first derivative of (2.13) with respect to <img src="14-1500105\f7776018-5c9d-43d9-bfc9-794980703284.jpg" /> for <img src="14-1500105\c8eadfda-3a69-4077-ad6c-8e8434705ff6.jpg" /> is as follows:</p><disp-formula id="scirp.19296-formula35273"><label>. (2.20)</label><graphic position="anchor" xlink:href="14-1500105\714362cf-568a-4374-ac3f-0165cae4c8cb.jpg"  xlink:type="simple"/></disp-formula><p>It is conceivable that the discussions for the GMM estimator based on the HTD transformation could be permitted to be conducted on the basis of numbers of observations for which <img src="14-1500105\f3e6688e-157d-49db-bf2b-0091f5b4dd5a.jpg" /> instead of<img src="14-1500105\27081cd9-d73b-43e3-8f2c-fa43fcedee65.jpg" />, on the grounds that observations except for those for which <img src="14-1500105\3cddfada-9caa-4ec0-bf15-b64ae1ce3f22.jpg" /> make no direct contribution to estimating<img src="14-1500105\3f8f8efd-6e41-44a5-9dfe-ee245b741133.jpg" />.</p><p>In this case, <img src="14-1500105\857c3c7f-0d81-4222-9d2f-da2583950d5e.jpg" />is expediently used instead of <img src="14-1500105\1158a6e3-4388-4cf3-9c06-84db95b88401.jpg" /> in this section, where <img src="14-1500105\c2ad207b-b065-4280-80a6-d94d84a49aed.jpg" /> is number of observations for which <img src="14-1500105\48f406a4-c35b-49ba-9155-42cf4712e961.jpg" /> at time<img src="14-1500105\af14f406-2649-41cf-b9f6-2f69e80918a5.jpg" />.</p></sec><sec id="s3"><title>3. Link between CMLE and GMM Estimator</title><p>The discussion here is conducted for the case of two periods (i.e. <img src="14-1500105\13c2299d-3fd5-48c4-a655-6e4ce5876ae1.jpg" />and<img src="14-1500105\357ae7d8-cf95-46a6-b7f5-2133adbbc620.jpg" />). It is shown in this section that the GMM estimator opting for an instrument is identical to the CMLE in this case.</p><p>First, the GMM estimator is presented. With <img src="14-1500105\3e27b2e8-7ef9-4b51-9d25-03b8b414fb49.jpg" /> and <img src="14-1500105\3038b6c8-23a2-4b99-9f29-eb53f5455d47.jpg" /> (both of which are scalars), Equation (2.13) turns to</p><disp-formula id="scirp.19296-formula35274"><label>. (3.1)</label><graphic position="anchor" xlink:href="14-1500105\04c1cf61-2fd5-433e-8fd0-d0221ef77b78.jpg"  xlink:type="simple"/></disp-formula><p>The moment condition (3.1) says that <img src="14-1500105\15dcfb69-3e9e-42fb-9f8c-e07140e1f939.jpg" /> is used as the instrument for the HTD transformation<img src="14-1500105\5722c33b-5dde-4750-8d44-f99d357085a1.jpg" />. The GMM estimator for <img src="14-1500105\ffd33a9e-4f44-4a2a-be78-ed55aa44525b.jpg" /> is the just-identified one when using only the moment condition (3.1) for the two periods. This is denoted by <img src="14-1500105\bdd87331-d047-4a2b-8834-0dc1828ebcc8.jpg" /> hereafter.</p><p>The first derivative of <img src="14-1500105\e9b85b34-6bdf-4502-9b1a-afff8dcf5117.jpg" /> with respect to <img src="14-1500105\ca205a6c-6a45-4f1a-abec-8720a769a498.jpg" /> and the square of <img src="14-1500105\aced6cdc-0b31-4ed8-bb2e-b1b759762d74.jpg" /> are respectively calculated as follows:</p><disp-formula id="scirp.19296-formula35275"><label>(3.2)</label><graphic position="anchor" xlink:href="14-1500105\acb01db3-4e0a-415d-99b0-afd9b645663a.jpg"  xlink:type="simple"/></disp-formula><p>and</p><disp-formula id="scirp.19296-formula35276"><label>(3.3)</label><graphic position="anchor" xlink:href="14-1500105\f13d118e-8eea-4a85-a9cb-d9d43dcc5623.jpg"  xlink:type="simple"/></disp-formula><p>where the relationship that <img src="14-1500105\43a52942-a548-4ec0-9203-3cb198242f08.jpg" /> if <img src="14-1500105\68e05c5f-7fa4-4a5e-9e88-c026f2bb3e31.jpg" /> is even and <img src="14-1500105\8c46c848-b2ff-48cc-8fc1-39aabbf83100.jpg" /> if <img src="14-1500105\741af255-9c46-4841-808a-5a9635919a6d.jpg" /> is odd is used since <img src="14-1500105\cece404d-cd1f-4ec8-b618-ec245b3fec8f.jpg" /> is binary. Using (2.19), (2.20), (3.2), and (3.3), <img src="14-1500105\414f592e-1ac5-42b0-ba46-4fa3f554238b.jpg" />and <img src="14-1500105\c76458a0-6ba0-4c3e-bb12-d91edd879ed0.jpg" /> for (3.1) are respectively calculated as follows:</p><disp-formula id="scirp.19296-formula35277"><label>(3.4)</label><graphic position="anchor" xlink:href="14-1500105\73b05dd2-82d9-4aa1-93ca-029ca059755d.jpg"  xlink:type="simple"/></disp-formula><p>where <img src="14-1500105\ceb555b8-4674-4dd1-b61e-ed4a41ffbcf1.jpg" /> is usedwhich is obtained from (2.11), and</p><disp-formula id="scirp.19296-formula35278"><label>(3.5)</label><graphic position="anchor" xlink:href="14-1500105\5d9a8acf-c3bc-4ada-a15e-692d5890436f.jpg"  xlink:type="simple"/></disp-formula><p>Looking at (3.4) and (3.5), it can be seen that</p><disp-formula id="scirp.19296-formula35279"><label>. (3.6)</label><graphic position="anchor" xlink:href="14-1500105\4d8241b9-5b6e-4d13-802f-15b086d8eeec.jpg"  xlink:type="simple"/></disp-formula><p>In addition, the relationship (2.18) is also applicable to the just-identified estimator (see pp. 486-487 in Hayashi, 2000, [<xref ref-type="bibr" rid="scirp.19296-ref23">23</xref>]). Therefore, it follows from (2.18) and (3.6) that the following relationship holds for<img src="14-1500105\d9d2f14f-ee66-41b0-b195-6c6cff9f6af5.jpg" />:</p><disp-formula id="scirp.19296-formula35280"><label>. (3.7)</label><graphic position="anchor" xlink:href="14-1500105\ceb9a5fa-a427-4337-8be2-54467d4580be.jpg"  xlink:type="simple"/></disp-formula><p>Lee (2002, pp. 84-87) [<xref ref-type="bibr" rid="scirp.19296-ref24">24</xref>] elucidates the equality conceptually identical to (3.6) in the context of the CMLE to be hereafter described. In addition, Bonhomme (2012) [<xref ref-type="bibr" rid="scirp.19296-ref25">25</xref>] demonstrates that the conditional moment restriction which he proposes for the fixed effects logit model can give birth to the unconditional moment condition identical to (3.1).</p><p>Next, the conventional CMLE proposed by Chamberlain (1980) [<xref ref-type="bibr" rid="scirp.19296-ref1">1</xref>] is presented for the two periods as follows:</p><disp-formula id="scirp.19296-formula35281"><label>, (3.8)</label><graphic position="anchor" xlink:href="14-1500105\3fd0e860-17ac-4825-b5ff-37349a7f1ef9.jpg"  xlink:type="simple"/></disp-formula><p>where<img src="14-1500105\41a89275-386d-45b5-ae88-65da4773c270.jpg" />. Referring to Wooldridge</p><p>(2002, pp. 490-492) [<xref ref-type="bibr" rid="scirp.19296-ref26">26</xref>], the logarithm of probability composing the conditional log-likelihood function for the two-periods fixed effects logit model is written as follows, with<img src="14-1500105\baedd866-aaf5-4e87-b0cb-be6b2f2b0bd1.jpg" />:</p><disp-formula id="scirp.19296-formula35282"><label>, (3.9)</label><graphic position="anchor" xlink:href="14-1500105\40ae1cee-c536-4915-8cb9-37e548a00130.jpg"  xlink:type="simple"/></disp-formula><p>where <img src="14-1500105\d6315140-cfb0-49c1-9936-995c5b71a475.jpg" /> if <img src="14-1500105\e03cef9d-46dc-4ba3-b491-ca97e9e84165.jpg" /> and <img src="14-1500105\f0e1caf4-f613-455e-b24b-3365645e5e97.jpg" /> otherwise, while <img src="14-1500105\2e19f9f5-5d8a-4e0f-acdc-c809bd6fb7a0.jpg" /> if <img src="14-1500105\cad680b0-03b8-432a-890a-97287a1a79f4.jpg" /> and <img src="14-1500105\36040201-b186-480a-b196-decb5e75ef63.jpg" /> and <img src="14-1500105\814c056f-2e33-45d9-8959-c2dfaa81ee03.jpg" /> if <img src="14-1500105\31cf0cb2-9c98-42df-822d-efdf5c5dc6d7.jpg" /> and<img src="14-1500105\f3377c22-77ce-4edf-8f8b-fdfdedc11fab.jpg" />. In (3.9), <img src="14-1500105\d9fc6fe6-8fba-4053-bf02-97d3fcfc733f.jpg" />stands for the probability with which <img src="14-1500105\ca7f298e-f7fb-4f10-a7ac-4421121e1530.jpg" /> takes one given<img src="14-1500105\3f3c2514-a9d9-4c7e-bcfc-a4a5a687bc31.jpg" />, <img src="14-1500105\8cc4b86a-118b-4a96-9bfb-00f2767d4d05.jpg" />, <img src="14-1500105\27790970-b772-4ccd-b403-945213c4aa9a.jpg" />and<img src="14-1500105\5c51076d-ed0d-4e55-96c7-907c453d775e.jpg" />, while <img src="14-1500105\f93abd04-7473-49e4-ab5a-a35d021facd5.jpg" /> stands for the probability with which <img src="14-1500105\1feabb5a-4024-481c-93d7-cebb93bb8d6c.jpg" /> takes zero given<img src="14-1500105\a94137d9-91a8-4933-8338-12e4eb0315e3.jpg" />, <img src="14-1500105\49a3c709-6a78-4750-a6ba-4582452c63ff.jpg" />, <img src="14-1500105\cd10769f-e5ef-4a42-9ccb-658c0d4309ae.jpg" />and<img src="14-1500105\c1462677-3998-4f25-b124-ee0767de3ecd.jpg" />.</p><p>The first-order condition of <img src="14-1500105\40bff849-77ef-41ff-a474-6442ce2b0c39.jpg" /> is</p><disp-formula id="scirp.19296-formula35283"><label>(3.10)</label><graphic position="anchor" xlink:href="14-1500105\18020141-e0ad-443b-8bb7-05278a894757.jpg"  xlink:type="simple"/></disp-formula><p>with</p><disp-formula id="scirp.19296-formula35284"><label>(3.11)</label><graphic position="anchor" xlink:href="14-1500105\610bf8e9-531e-4dee-a6d6-0a6813da9037.jpg"  xlink:type="simple"/></disp-formula><p>It is corroborated from (3.10) with (3.11) that the first-order condition of <img src="14-1500105\c0ae3e8d-a10a-485d-8b0b-172ecda52f7b.jpg" /> divided by <img src="14-1500105\91f6077a-3fd9-4120-b639-423d945df0ea.jpg" /> is the empirical counterpart of the moment condition (3.1) for the GMM estimator. The second-order derivative of <img src="14-1500105\a5e91716-6c1c-4379-a9de-f0e5ad417aaa.jpg" /> with respect to <img src="14-1500105\45d12f81-ffa4-43ed-b011-49df17c34bc5.jpg" /> is written as</p><disp-formula id="scirp.19296-formula35285"><label>(3.12)</label><graphic position="anchor" xlink:href="14-1500105\5dc3d21a-5e2d-42f4-bd5a-01713cf0b9a1.jpg"  xlink:type="simple"/></disp-formula><p>Taking notice of the fact that</p><p><img src="14-1500105\53dd0cbb-50f9-45a9-a7fb-5a2a552e78aa.jpg" />, it is evident that if <img src="14-1500105\52b50607-4b41-4e25-ad13-dfe33b7fa67c.jpg" /> is replaced by<img src="14-1500105\e9be873b-8d12-4225-90d8-ddd47899485f.jpg" />, (3.12) divided by <img src="14-1500105\d8e45014-206c-42dc-a117-fc8413ec3580.jpg" /> is the empirical counterpart of (3.5) and accordingly identical to <img src="14-1500105\6a1a9299-4d77-4db3-b2a2-0c269ba7125d.jpg" /> from (3.6). Therefore, the following relationship holds for<img src="14-1500105\e146cd9e-9c5e-4152-921c-373329fa24e9.jpg" />:</p><disp-formula id="scirp.19296-formula35286"><label>. (3.13)</label><graphic position="anchor" xlink:href="14-1500105\a3dd936e-cf3d-4eef-b142-bb64a7838580.jpg"  xlink:type="simple"/></disp-formula><p>Judging from the above, it is ascertained that for the two periods the conventional CMLE for the fixed effects logit model is identical to the GMM estimator selecting <img src="14-1500105\01fd2ba9-1759-4805-b0ec-51b523c136a5.jpg" /> as the instrument for the HTD transformation.</p><p>To make doubly sure, the integration of</p><p><img src="14-1500105\b554362a-f739-458e-be2f-0afcb1e0a474.jpg" />with respect to <img src="14-1500105\e1757b83-3dfa-45db-8a60-83f259f05a24.jpg" /> is conducted:</p><disp-formula id="scirp.19296-formula35287"><label>(3.14)</label><graphic position="anchor" xlink:href="14-1500105\d3176518-fa3b-4a38-a92c-373af1670a9f.jpg"  xlink:type="simple"/></disp-formula><p>where <img src="14-1500105\0964d439-c291-42e5-be10-8a5c1f131d1d.jpg" /> is the constant of integration. With <img src="14-1500105\6602c609-1474-4a71-a4c5-d99382c8691b.jpg" /> for (3.14), the logarithm of probability (3.9), which composes the conditional log-likelihood function for the two-periods fixed effects logit model, is compactly rewritten as</p><disp-formula id="scirp.19296-formula35288"><label>(3.15)</label><graphic position="anchor" xlink:href="14-1500105\c31dabac-cc9c-4277-b6b0-68c3b6b92651.jpg"  xlink:type="simple"/></disp-formula><p>The exponential of <img src="14-1500105\fa80f5f6-46ea-47ec-8127-230a4871eb66.jpg" /> in (3.15), which is equivalent to (3.9), represents the probability density when the restriction <img src="14-1500105\2635bae0-06a6-4f80-af4b-4e43a1801518.jpg" /> is imposed. In this case, number of observations for which <img src="14-1500105\c4fa6277-ab9e-4521-802e-9ea23ef11a2e.jpg" /> is used instead of <img src="14-1500105\b211b68d-8c1a-4d83-8a27-7a5b99b3d110.jpg" /> in this section and therefore<img src="14-1500105\8cbfe407-dd6c-4524-8683-021f64941872.jpg" />, which is equivalent to<img src="14-1500105\1ac11829-e37f-41a6-a8d8-6440b54c9d19.jpg" />, could be interpreted as being the asymptotically efficient estimator. This is because the Cram&#233;rRao inequality is applicable in this case.</p><p>Incidentally, Abrevaya (1997) [<xref ref-type="bibr" rid="scirp.19296-ref27">27</xref>] shows that for the fixed effects logit model, a scale-adjusted ordinary maximum likelihood estimator is equivalent to the CMLE for the case of two periods.</p></sec><sec id="s4"><title>4. Monte Carlo</title><p>In this section, some Monte Carlo experiments are conducted to investigate the small sample performance of the GMM estimator for the fixed effects logit model described in Section 2. The experiments are implemented by using an econometric software TSP version 4.5 (see Hall and Cummins, 2006, [<xref ref-type="bibr" rid="scirp.19296-ref28">28</xref>]).</p><p>The data generating process (DGP) is as follows:</p><p><img src="14-1500105\e34e65e3-94ef-4e2f-b83f-3d57def54cab.jpg" />,</p><p><img src="14-1500105\a395ecf5-a2e3-4b70-b904-53b8fc649841.jpg" />,</p><p><img src="14-1500105\8fe4753b-8a98-4380-8cd4-0465eb6cd0bc.jpg" />,</p><p><img src="14-1500105\ad6ec7bd-43c4-45ae-b30b-f3ed5bf15c74.jpg" />,</p><p><img src="14-1500105\cb0d404e-3d19-4fd4-bfeb-9e0a901ce316.jpg" />,</p><p><img src="14-1500105\3beaf4d3-70f3-4277-8791-7584c63251b9.jpg" />;<img src="14-1500105\8a4f64cc-5d22-4e0a-8b89-12c4de6e5787.jpg" />.</p><p>In the DGP, values are set to the parameters<img src="14-1500105\b003b1c7-e33d-4512-bd73-765faa3feb48.jpg" />, <img src="14-1500105\f5791d50-5e3b-4d8c-8e85-1002b63f5685.jpg" />, <img src="14-1500105\8a1e78bc-a622-4306-a748-783231171c15.jpg" />, <img src="14-1500105\b4e4ae09-754d-40a9-abc8-ad9efcac3cb2.jpg" />and<img src="14-1500105\d4eb028c-56b1-4c0a-a0f3-6eb7a18b3355.jpg" />. The experiments are carried out with the cross-sectional sizes<img src="14-1500105\7b9c9544-0718-4ccf-9221-137f374fd124.jpg" />, <img src="14-1500105\d270b71f-0d6b-4faf-9615-da9eb34a81f9.jpg" />and<img src="14-1500105\56b36060-4d0c-4fa2-9d3d-9821e7c0f6bc.jpg" />, the numbers of time periods<img src="14-1500105\d927b11b-8f5c-41c7-bc84-a3974a78fc73.jpg" />, <img src="14-1500105\2cf2b992-264e-4611-a24b-df0c82e98b4d.jpg" />and<img src="14-1500105\03aa3170-e1ae-4316-9856-057bd13f1f72.jpg" />, and the number of replications<img src="14-1500105\4be8b710-88d8-4f57-8c06-dce12031dad1.jpg" />.</p><p>In the experiments, the GMM estimator based on the HTD transformation selects <img src="14-1500105\93038891-5adc-4b35-b870-e737e7353ad2.jpg" /> as the instruments for the transformation<img src="14-1500105\69277ce2-aa9a-49f6-b4e2-cc1cf365f0c0.jpg" />. That is, the GMM(HTD) estimator uses the vector of moment conditions (2.13) with<img src="14-1500105\01075c63-70c0-4777-a98a-6be3a713f5ad.jpg" />, which is able to be written piecewise as follows:</p><p><img src="14-1500105\a2964fbc-3df4-4423-906b-7b19e78e6638.jpg" />, for<img src="14-1500105\b1100f16-1264-4d47-83e3-baf8b8191096.jpg" />.<sup>8</sup> (4.1)</p><p>As a control, another GMM estimator is used, which employs the following moment conditions disregarding the unobservable heterogeneity:</p><p><img src="14-1500105\4d9225cf-b8e6-4aa1-a18b-f64771a86d11.jpg" />, for<img src="14-1500105\c613055e-ec31-45c1-abfe-718e9dc00783.jpg" />. (4.2)</p><p>where<img src="14-1500105\03c98dcf-0080-4a6f-a380-777087ed52ed.jpg" />. The GMM (LgtLev) estimator (i.e. the level GMM estimator for the logit model) for <img src="14-1500105\7ec63dd0-0e38-446f-98d8-017da69c2b3b.jpg" /> is inconsistent due to the ignorance of the fixed effects.</p><p>The Monte Carlo results are exhibited in <xref ref-type="table" rid="table1">Table 1</xref>. The settings of values of the parameters for the explanatory variables <img src="14-1500105\68f3029f-3e7d-4d7e-a997-e232f836b78b.jpg" /> are the same as those used by Blundell et al. (2002) [<xref ref-type="bibr" rid="scirp.19296-ref21">21</xref>] for count panel data model. The small sample property of the GMM(HTD) estimator can be said to be preferable and their bias and rmse (root mean squared error) decrease as the cross-sectional size <img src="14-1500105\896310b2-929a-4b64-8c93-01e941f3a3f4.jpg" /> increases, which is the reflection of the consistency. In contrast, the sizable downward bias and rmse for the (inconsistent) GMM(LgtLev) estimator remain at virtually constant levels when <img src="14-1500105\9b6bc70e-4d01-4d79-9fa9-b9819acc19e1.jpg" /> increases. As is seen from comparisons among Simulations (a4), (a8) and (a25), among Simulations (b4), (b8) and (b25), and Simulations (c4), (c8) and (c25) for the GMM(HTD) estimator, the small sample performance of the GMM(HTD) estimator is better off as the number of time periods increases, reflecting the substantive increase of sample size. Furthermore, comparisons among Simulations (a4), (b4) and (c4), among Simulations (a8), (b8) and (c8), and among Simulations (a25), (b25) and (c25) for the GMM(HTD) estimator raise the possibility that more persistent series of the explanatory variables might bring about more deteriorated small sample performance of the GMM(HTD) estimator.9</p><table-wrap-group id="1"><label><xref ref-type="table" rid="table1">Table 1</xref></label><caption><title> Monte Carlo results for the fixed effects logit model</title></caption></table-wrap-group></sec><sec id="s5"><title>5. Average Elasticity</title><p>For the fixed effects logit model composed of (2.1) and (2.2), the new index is constructed by using both the consistent estimator for <img src="14-1500105\94a8f572-1013-4630-b5a1-776543eb9b2b.jpg" /> described in previous sections and the average of<img src="14-1500105\3a5b3551-3112-4bd8-8059-a22f18d8b47d.jpg" />. The average elasticity of the logit probability with respect to the exponential function of explanatory variable (which is calculated without relation to the fixed effects) is an appropriate index in the framework of the fixed effects logit model with time dimension being strictly fixed, where no (consistent) average marginal effect is available.1<sup>0</sup> In this section, the assumption that the variables are identically distributed among individuals is unfastened.1<sup>1</sup></p><p>With<img src="14-1500105\b7ff1601-af6d-4d31-8f3c-8b1874ae7616.jpg" />, the elasticity of the probability <img src="14-1500105\806a4338-949a-4f90-90ba-9f05b253cdaa.jpg" /> with respect to the positive-valued variable <img src="14-1500105\31c5edd1-b5d8-4678-8b80-ceb643face3e.jpg" /> (with <img src="14-1500105\30f22d6e-034c-4932-99f8-2935fa724979.jpg" /> being held constant) is defined as follows:</p><p><img src="14-1500105\e05a6e15-b346-47ce-93bf-ea9c57b2728f.jpg" />for</p><disp-formula id="scirp.19296-formula35289"><label>. (5.1)</label><graphic position="anchor" xlink:href="14-1500105\2fee3e45-3ca9-4c22-8865-a898784ef4b1.jpg"  xlink:type="simple"/></disp-formula><p>Under the assumption that<img src="14-1500105\6eeaa28b-9bd0-4356-82d7-9c33a9053108.jpg" />, the overall average elasticity of <img src="14-1500105\fcc8a571-2c5d-4eca-8946-6dbf3be10e56.jpg" /> with respect to <img src="14-1500105\f8c6e6c4-0f9a-4504-93e8-ecd7662a0d02.jpg" /> is calculated with the following formula:</p><disp-formula id="scirp.19296-formula35290"><label>, (5.2)</label><graphic position="anchor" xlink:href="14-1500105\97ea9a59-f513-446a-8664-890332d4e82e.jpg"  xlink:type="simple"/></disp-formula><p>where <img src="14-1500105\3db1b5d6-daee-401e-839b-068fe58d17d6.jpg" /> is the consistent estimator for <img src="14-1500105\01c814ba-f7a3-4bc8-8694-af28fe1a67a4.jpg" /> such that</p><p><img src="14-1500105\c93cdff2-4713-4aab-8687-ac5b1871c1c6.jpg" />and<img src="14-1500105\aff4f35e-b69b-438c-893a-de11faeaeaa6.jpg" />. Since</p><p><img src="14-1500105\bef896da-80d8-4455-8aa1-2a2e51dfe269.jpg" />is the probability and <img src="14-1500105\900950c8-d6af-40d8-ba37-c966fb60fd02.jpg" /> (and accordingly variances of <img src="14-1500105\a2bd0158-bbdf-49eb-b5e8-565ae5ed49ec.jpg" /> are finite), it can be seen that<img src="14-1500105\905b4971-4950-48df-bb15-16450e644491.jpg" />, if</p><p><img src="14-1500105\c2a08772-11a2-4543-9f91-4cd01a98f839.jpg" />(which is referred to as the average logit probability in this paper).1<sup>2</sup></p><p>In addition, the cross-section average elasticity for a specific time period and the group average elasticity for a group (e.g. a gender) are able to be calculated as follows, respectively: The formula calculating the cross-section average of <img src="14-1500105\783e4d94-52b6-442c-b156-424a0a320db3.jpg" /> with respect to <img src="14-1500105\ce44e873-b68f-439b-838c-85f6473f6c5a.jpg" /> for period <img src="14-1500105\0e742163-855f-4850-a47e-beb915c5ef30.jpg" /> is</p><disp-formula id="scirp.19296-formula35291"><label>, (5.3)</label><graphic position="anchor" xlink:href="14-1500105\0c9f540b-0fa6-4a4a-b023-8677978941b0.jpg"  xlink:type="simple"/></disp-formula><p>where<img src="14-1500105\d5132f21-740a-4f30-b256-2a790dbd72d2.jpg" />, while that calculating the group average elasticity for group <img src="14-1500105\af8af006-db76-4008-82c8-e7e0423b591d.jpg" /> in population is</p><disp-formula id="scirp.19296-formula35292"><label>, (5.4)</label><graphic position="anchor" xlink:href="14-1500105\b38eb274-cd43-4f12-8e73-a43dd9922846.jpg"  xlink:type="simple"/></disp-formula><p>where <img src="14-1500105\404abef4-e8bc-4ebc-8947-269c19ae0b42.jpg" /> with subscript <img src="14-1500105\03917edc-2ba8-4e0d-96ee-422bcfbc4c67.jpg" /></p><p>denoting the member of group<img src="14-1500105\18c76bb5-3556-4f46-8db2-488c87046d66.jpg" />, <img src="14-1500105\e485d7db-9a10-4208-afb7-b58c5f982d25.jpg" />being number of individual units belonging to group<img src="14-1500105\996b86de-5c56-4ffe-85d2-f19a61da8ca2.jpg" />, and <img src="14-1500105\5d0a6103-414f-404b-b1b6-cb44a535471a.jpg" /> being the binary dependent variable for the individual <img src="14-1500105\a7120484-2b42-4efe-aed7-8824ef194619.jpg" /> appertaining to group <img src="14-1500105\90e9baa7-8f7c-45aa-955c-319c9a5ea882.jpg" /> at period<img src="14-1500105\bc7cb879-cc55-4578-9146-3ca398c51052.jpg" />.</p></sec><sec id="s6"><title>6. Conclusion</title><p>This paper proposed the hyperbolic tangent differencing (HTD) transformation for the fixed effects logit model, with the intention of ruling out the fixed effects. The consistent GMM estimator was constructed by using the HTD transformation. The equivalence of the GMM estimator opting for an instrument and the CMLE proposed by Chamberlain (1980) [<xref ref-type="bibr" rid="scirp.19296-ref1">1</xref>] was revealed for the case of two periods. Then, the Monte Carlo experiments indicated the desirable small sample property of the GMM estimator based on the HTD transformation. In addition, the average elasticity of the logit probability with respect to the exponential function of explanatory variable was proposed, which is an appropriate index from the point of view that it is able to be calculated without the fixed effects. Both of the simple estimator and index will facilitate empirical researchers exploring the binary choice panel data model.</p></sec><sec id="s7"><title>REFERENCES</title></sec><sec id="s8"><title>NOTES</title></sec></body><back><ref-list><title>References</title><ref id="scirp.19296-ref1"><label>1</label><mixed-citation publication-type="other" xlink:type="simple">G, Chamberlain, “Analysis of Covariance with Qualitative Data,” Review of Economic Studies, Vol. 47, No. 1, 1980, pp. 225-238. doi:10.2307/2297110</mixed-citation></ref><ref id="scirp.19296-ref2"><label>2</label><mixed-citation publication-type="other" xlink:type="simple">J. Neyman and E. L. 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