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>> No.11495802 [View]
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11495802

>>11495790
That's pretty neat. I've also heard form a friend that any 1 and 2D quantum order can be simulated with a space of localized quantum dots and you by tuning interaction parameters, I guess this is similar. Though maintaining the coherence of local quantum dots is pretty taxing.
Thanks for the links, I'll have another thing to talk about with my cond mat sims colleagues

>> No.11389984 [View]
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11389984

>>11389393
Fuck yeah this is a good one.

>> No.11065753 [View]
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11065753

>>11065746
It makes formalizing Lagrangian density straightforward. [math]\mathcal{L}[/math] is just a [math]d[/math]-form on the jet bundle, where [math]d = \operatorname{dim}M[/math]. The action is then "just" the "de-Rham" pairing [math]\langle M,\mathcal{L}\rangle = \int_M \mathcal{L}[/math].

>> No.9076624 [DELETED]  [View]
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9076624

>>9072120
Talk to one of the profs you know and do a thesis class with him as supervisor. If you can't then just do something with him informal on the side over the next semester. This way he can at least write you a unique recommendation letter for employers/grad admission.

>> No.9047097 [View]
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9047097

>>9046804
>What's your favorite number theorem in number theory, anons?
Let [math]\zeta_{k_1\dots k_n} = \sum_{m_1 < \dots < m_n}\frac{1}{m_1^{k_1} \dots m_n^{k_n}}[/math] be the multiple zeta function, then [math]\zeta_{1,2} = \zeta_3[/math].

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