sommerfeld method 11.10.2010.docx

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    Previous lecture 2010.09.29 Next lecture 2010.10.13 to index

    Sommerfeld Method 11.10.2010

    We have repeated the last lecture with stress on this:

    How to

    so_0.pngThe main point is evaluating the N(E) (number of accomodated electrons) up to a given E (energy)The colored "expression" can be anything in the sum (integral) above

    The argumet goes like this:

    sum -> sum with the proper deltas which are compensated by the 1/Deltas outside the sum

    Then keep the 1/Deltas outside the sumand concentrate on the Sum with deltas; Taking this by itself, it will converge to an integral

    when you make Deltas infinitesimalThe Deltas outside are not to be made infinitesimal, SINCE they connect to the original sum

    http://web.ift.uib.no/AMOS/PHYS208/2010.09.29/index.htmlhttp://web.ift.uib.no/AMOS/PHYS208/2010.09.29/index.htmlhttp://web.ift.uib.no/AMOS/PHYS208/2010.10.13/index.htmlhttp://web.ift.uib.no/AMOS/PHYS208/2010.10.13/index.htmlhttp://web.ift.uib.no/AMOS/PHYS208/index.htmlhttp://web.ift.uib.no/AMOS/PHYS208/index.htmlhttp://web.ift.uib.no/AMOS/PHYS208/index.htmlhttp://web.ift.uib.no/AMOS/PHYS208/2010.10.13/index.htmlhttp://web.ift.uib.no/AMOS/PHYS208/2010.09.29/index.html
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    This is sometimes not so easy to keep in mind .... ( the sum itself would go to infinity ... )

    From this follows the dependence of Fermi energy on N/V - the density (see last time ... )

    We have also played with the Fermi Function matlab program(showing that the parameter mu can be adjusted in iterations- the program sums the occupation numbers - adjust mu - and stops when the Sum is equal the number of electrons

    The program will be especially interesting later - with ENERGY GAP)../FERMI/Fermi function Matlab toys ( ferm2.m and fermgap.m - the others are older versions and other scripts)

    http://web.ift.uib.no/AMOS/PHYS208/FERMI/http://web.ift.uib.no/AMOS/PHYS208/FERMI/http://web.ift.uib.no/AMOS/PHYS208/FERMI/
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    Sommerfeld method for evaluation of integrals with Fermi DistributionRecord of the lecture follows,

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    more details are given in the scans below this note (which we discussed in the lecture)

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    so_1.png

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    so_2.png

    The above formula can be viewed as a method. It is applicable to any of the necessary expressions,involving either g(E) or Eg(E)

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    so_3.pngHere we have summarized also the final result from the notes belowThe heat capacity is indeed proportional to the ratio T / TF - and TF is VERY BIG so that heat capacity is very SMALL(about 100 times smaller than the classical one

    Note - the heat capacity is LINEARY dependent on T. For PHONONS it was dependent (Debye) on T3

    Thus, there will allways be a region of very small temperatures where AT is larger than B T3 (which region depends on A,B )

    So for normal temperatures, the electron contribution to C (heat capacity) is negligibleBut for extremely low temperatures it becomes dominating

    The Sommerfeld method - details are in the three scans below

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    EVALUATION SCAN

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    In this scan the evaluation is summarized with all the extra approximation highlighted

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    In the last based on exam texts the whole story is also summarized

    EXAMS 1990-2000 - text copied

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    to_1.png

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    to_2.png

    to_3.png

    Previous lecture 2010.09.29 Next lecture 2010.10.13

    http://web.ift.uib.no/AMOS/PHYS208/2010.09.29/index.htmlhttp://web.ift.uib.no/AMOS/PHYS208/2010.09.29/index.htmlhttp://web.ift.uib.no/AMOS/PHYS208/2010.10.13/index.htmlhttp://web.ift.uib.no/AMOS/PHYS208/2010.10.13/index.htmlhttp://web.ift.uib.no/AMOS/PHYS208/2010.10.13/index.htmlhttp://web.ift.uib.no/AMOS/PHYS208/2010.09.29/index.html