• About the partial differential symbol used by F. Duncan M. Haldane.

    From Hongyi Zhao@21:1/5 to All on Mon Jul 12 18:06:05 2021
    Haldane gave a talk on his 2012 ICTP Dirac Medal, of which the
    corresponding presentation can be retrieved online from <https://physics.princeton.edu//~haldane/talks/dirac.pdf>. On the
    page 6 of this talk in the above-mentioned file, he wrote the
    following formula:

    \left|\partial_{\mu} \Psi(\boldsymbol{x})\right\rangle \equiv
    \sum_{i} \frac{\partial u_{i}(\boldsymbol{x})}{\partial x^{\mu}}|i\rangle

    But I'm confused on the symbols used here. Any more hints/explanations
    willl be highly appreciated.

    Regards,
    HY

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  • From Jos Bergervoet@21:1/5 to Hongyi Zhao on Tue Jul 13 08:49:05 2021
    On 21/07/13 3:06 AM, Hongyi Zhao wrote:
    Haldane gave a talk on his 2012 ICTP Dirac Medal, of which the
    corresponding presentation can be retrieved online from <https://physics.princeton.edu//~haldane/talks/dirac.pdf>. On the
    page 6 of this talk in the above-mentioned file, he wrote the
    following formula:

    \left|\partial_{\mu} \Psi(\boldsymbol{x})\right\rangle \equiv
    \sum_{i} \frac{\partial u_{i}(\boldsymbol{x})}{\partial x^{\mu}}|i\rangle

    But I'm confused on the symbols used here. Any more hints/explanations
    willl be highly appreciated.

    Regards,
    HY


    It seems to be factoring of the total wave function
    Psi into a spinor part |i> and a spatial part u_i(x),
    where the summation index i is then over the number
    of spin states.

    It is then assumed that the space-time-dependence is
    through the u_i(x) and that the |i> are fixed in time.

    --
    Jos

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  • From Hongyi Zhao@21:1/5 to Jos Bergervoet on Tue Jul 13 20:12:03 2021
    On Tuesday, July 13, 2021 at 4:49:08 PM UTC+8, Jos Bergervoet wrote:
    On 21/07/13 3:06 AM, Hongyi Zhao wrote:
    Haldane gave a talk on his 2012 ICTP Dirac Medal, of which the corresponding presentation can be retrieved online from <https://physics.princeton.edu//~haldane/talks/dirac.pdf>. On the
    page 6 of this talk in the above-mentioned file, he wrote the
    following formula:

    \left|\partial_{\mu} \Psi(\boldsymbol{x})\right\rangle \equiv
    \sum_{i} \frac{\partial u_{i}(\boldsymbol{x})}{\partial x^{\mu}}|i\rangle

    But I'm confused on the symbols used here. Any more hints/explanations willl be highly appreciated.

    Regards,
    HY

    It seems to be factoring of the total wave function
    Psi into a spinor part |i> and a spatial part u_i(x),

    How do you deduce that |i> is a spinor part and u_i(x) is a spatial
    part? Based on the talk file given on the website, I can only see
    that |i> is a set of fixed orthonormal basis and u_i(x) is the i-th
    expanding coefficient of "\Psi x" on this basis.

    where the summation index i is then over the number
    of spin states.

    Again, based on the context of the formula, I can not see where the
    author speaks of a "spin state".

    It is then assumed that the space-time-dependence is
    through the u_i(x) and that the |i> are fixed in time.

    I really can't find this implication too.

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  • From Jos Bergervoet@21:1/5 to Hongyi Zhao on Wed Jul 14 09:39:03 2021
    On 21/07/14 5:12 AM, Hongyi Zhao wrote:
    On Tuesday, July 13, 2021 at 4:49:08 PM UTC+8, Jos Bergervoet wrote:
    On 21/07/13 3:06 AM, Hongyi Zhao wrote:
    Haldane gave a talk on his 2012 ICTP Dirac Medal, of which the
    corresponding presentation can be retrieved online from
    <https://physics.princeton.edu//~haldane/talks/dirac.pdf>. On the
    page 6 of this talk in the above-mentioned file, he wrote the
    following formula:

    \left|\partial_{\mu} \Psi(\boldsymbol{x})\right\rangle \equiv
    \sum_{i} \frac{\partial u_{i}(\boldsymbol{x})}{\partial x^{\mu}}|i\rangle >>>
    But I'm confused on the symbols used here. Any more hints/explanations
    willl be highly appreciated.

    Regards,
    HY

    It seems to be factoring of the total wave function
    Psi into a spinor part |i> and a spatial part u_i(x),

    How do you deduce that |i> is a spinor part and u_i(x) is a spatial
    part?

    I did not deduce that it is so with certainty (that is why I
    wrote *It seems* at the beginning). To me it seems the most
    straightforward interpretation without any further information,
    because such a factorization is quite usual.

    Based on the talk file given on the website, I can only see
    that |i> is a set of fixed orthonormal basis and u_i(x) is the i-th
    expanding coefficient of "\Psi x" on this basis.

    where the summation index i is then over the number
    of spin states.

    Again, based on the context of the formula, I can not see where the
    author speaks of a "spin state".

    It is then assumed that the space-time-dependence is
    through the u_i(x) and that the |i> are fixed in time.

    I really can't find this implication too.

    Again, this is not an implication, it is in my view a very likely
    explanation (and in OP you asked for *any* explanation!) You will
    have to look at the rest of the presentation for reasons to believe,
    or not believe this explanation.

    In any case we can conclude that it is a factorization of the state
    space where only the first part contains space-time dependence.
    And it contains a sum (as opposed to a single product of two factors)
    so it describes entangled states of the two parts. Making it highly
    suggestive that this is the splitting of spatial and internal degrees
    of freedom. Internal degrees of freedom most likely contain at least
    spin. But admittedly, there is no hard proof. Especially these |i>
    could contain more than only spin.

    One can also wonder why one part, u_i(x), is written as a function,
    and the other, |i>, uses Dirac notation. (But given the circumstances
    of the presentation, the author may have had other reasons for wanting
    to use the latter..)

    --
    Jos

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  • From Hongyi Zhao@21:1/5 to Jos Bergervoet on Wed Jul 14 23:14:42 2021
    On Tuesday, July 13, 2021 at 4:49:08 PM UTC+8, Jos Bergervoet wrote:
    On 21/07/13 3:06 AM, Hongyi Zhao wrote:
    Haldane gave a talk on his 2012 ICTP Dirac Medal, of which the corresponding presentation can be retrieved online from <https://physics.princeton.edu//~haldane/talks/dirac.pdf>. On the
    page 6 of this talk in the above-mentioned file, he wrote the
    following formula:

    \left|\partial_{\mu} \Psi(\boldsymbol{x})\right\rangle \equiv
    \sum_{i} \frac{\partial u_{i}(\boldsymbol{x})}{\partial x^{\mu}}|i\rangle

    But I'm confused on the symbols used here. Any more hints/explanations willl be highly appreciated.

    Regards,
    HY

    It seems to be factoring of the total wave function
    Psi into a spinor part |i> and a spatial part u_i(x),
    where the summation index i is then over the number
    of spin states.

    It is then assumed that the space-time-dependence is
    through the u_i(x) and that the |i> are fixed in time.

    The following it the explanation by Haldane himself, and I posted here,
    just FYI:

    ```
    partial_{\mu} means \frac{\partial}{\partial x^{\mu}}

    (contravariant and covariant index placement is being used)
    this is a standard notation in multidimensional differential geometry.
    (here the geometry of the parameter space x^{\mu}, \mu = 1,2--..D
    ```
    Regards,
    HY

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