﻿<?xml version="1.0" encoding="UTF-8"?>
<records>
  <record>
    <language>eng</language>
    <publisher>Science and Education Publishing</publisher>
    <journalTitle>International Journal of Physics</journalTitle>
    <eissn>2333-4576</eissn>
    <publicationDate>2015-02-25</publicationDate>
    <volume>3</volume>
    <issue>2</issue>
    <startPage>88</startPage>
    <endPage>95</endPage>
    <doi>10.12691/ijp-3-2-7</doi>
    <publisherRecordId>IJP2015327</publisherRecordId>
    <documentType>article</documentType>
    <title language="eng">Gapless Superconductivity</title>
    <authors>
      <author>
        <name>Boris V. Bondarev</name>
        <email>bondarev.b@mail.ru</email>
        <affiliationId>1</affiliationId>
      </author>
    </authors>
    <affiliationsList>
      <affiliationName affiliationId="1">Moscow Aviation Institute, VolokolamskoeShosse, 4, 125871, Moscow, Russia</affiliationName>
    </affiliationsList>
    <abstract language="eng">The mean field method is applied for analysis of valence electrons in metals. It is shown that at low temperatures electrons have two wave-vector distribution patterns. Isotropic distribution refers to the first pattern. Anisotropic distribution refers to another pattern, particularly to specific wave vector values occurred nearby the Fermi sphere. It is shown that it is the anisotropy that makes the metal obtain its specific superconductor features.</abstract>
    <fullTextUrl format="pdf">http://pubs.sciepub.com/ijp/3/2/7/ijp-3-2-7.pdf</fullTextUrl>
    <keywords language="eng">
      <keyword>valence electrons</keyword>
      <keyword>mean field method</keyword>
      <keyword>Fermi-Dirac function</keyword>
      <keyword>isotropic and anisotropic distributions</keyword>
      <keyword>superconductivity</keyword>
    </keywords>
  </record>
</records>