seminars:anal:2014_2015
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| + | ~~META: | ||
| + | --------- | ||
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| + | |||
| + | ---- | ||
| + | |||
| + | ====Fall 2025==== | ||
| + | |||
| + | |||
| + | |||
| + | |||
| + | * **August 20th, Wednesday ** (4: | ||
| + | **//Speaker //**: \\ | ||
| + | **// | ||
| + | \\ \\ | ||
| + | |||
| + | |||
| + | |||
| + | * **September 10th, Wednesday ** (4: | ||
| + | **// Speaker //**: Rohan Sarkar(Binghamton)\\ | ||
| + | **// | ||
| + | \\ \\ | ||
| + | <WRAP box 80%> | ||
| + | **// | ||
| + | whose spectral properties have been extensively studied over past few decades. Our main results show that, under suitable conditions on the Lévy process, the spectrum of the Lévy-OU semigroup in the $L^p$-space weighted with the invariant distribution coincides with that of the diffusion OU semigroup. Furthermore, | ||
| + | |||
| + | \\ | ||
| + | </ | ||
| + | \\ \\ | ||
| + | |||
| + | |||
| + | * **September 17th, Wednesday ** (4: | ||
| + | **//Speaker //**: Ziyao Xu (Binghamton) | ||
| + | **// | ||
| + | \\ \\ | ||
| + | <WRAP box 80%> | ||
| + | **// | ||
| + | \\ | ||
| + | </ | ||
| + | \\ \\ | ||
| + | |||
| + | |||
| + | |||
| + | * **September 24th, Wednesday ** (4: | ||
| + | **// Speaker //**: Rosh Hashanah break \\ | ||
| + | **// | ||
| + | \\ \\ | ||
| + | |||
| + | |||
| + | * **October 1st, Wednesday ** (4: | ||
| + | **// | ||
| + | **// | ||
| + | \\ | ||
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| + | |||
| + | * **October 8th, Wednesday ** (4: | ||
| + | **// | ||
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| + | \\ \\ | ||
| + | <WRAP box 80%> | ||
| + | **// | ||
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| + | </ | ||
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| + | * **October 30th, Thursday(Special date) ** (4: | ||
| + | **// | ||
| + | **// | ||
| + | |||
| + | \\ | ||
| + | <WRAP box 80%> | ||
| + | **// | ||
| + | |||
| + | </ | ||
| + | \\ \\ | ||
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| + | |||
| + | | ||
| + | **// | ||
| + | **// | ||
| + | |||
| + | \\ | ||
| + | <WRAP box 80%> | ||
| + | **// | ||
| + | Applications of our main result include the following: | ||
| + | |||
| + | (i) If the boundary $\partial D$ is sufficiently regular, then $D$'s area and $\partial D$'s length can both be recovered almost surely from a single observation of the AH's eigenvalues. | ||
| + | |||
| + | (ii) If $D$ is simply connected and $\partial D$ is fractal, then $\partial D$'s Minkowski dimension (if it exists) | ||
| + | can be recovered almost surely from the PAM's small-$t$ asymptotics. | ||
| + | |||
| + | (iii) The variance of the white noise can be recovered almost surely from a single observation of the AH's eigenvalues. | ||
| + | | ||
| + | \\ | ||
| + | </ | ||
| + | \\ \\ | ||
| + | |||
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| + | |||
| + | * **Room 309, November 20th, Thursday ** (4: | ||
| + | **// | ||
| + | **// | ||
| + | \\ | ||
| + | <WRAP box 80%> | ||
| + | **// | ||
| + | \\ | ||
| + | </ | ||
| + | \\ \\ | ||
| + | |||
| + | |||
| + | * **November 26th, Wednesday ** (4: | ||
| + | **// | ||
| + | **// | ||
| + | \\ | ||
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| + | |||
| + | |||
| + | * **December 3rd, Wednesday ** (4: | ||
| + | **// | ||
| + | **// | ||
| + | \\ | ||
| + | <WRAP box 80%> **// | ||
| + | |||
| + | |||
| + | \\ | ||
| + | </ | ||
| + | \\ \\ | ||
| + | |||
| + | |||
| + | |||
| + | |||
| + | ---- | ||
| + | |||
| + | ====Spring 2025==== | ||
| + | |||
| + | |||
| + | |||
| + | |||
| + | * **January 22nd, Wednesday ** (4-5pm)\\ | ||
| + | \\ \\ | ||
| + | <WRAP box 80%> **// | ||
| + | \\ | ||
| + | </ | ||
| + | \\ \\ | ||
| + | |||
| + | |||
| + | |||
| + | * **January 29th, Wednesday ** (4-5pm)\\ | ||
| + | \\ | ||
| + | \\ **// | ||
| + | \\ \\ | ||
| + | <WRAP box 80%> **// | ||
| + | |||
| + | \\ | ||
| + | </ | ||
| + | \\ \\ | ||
| + | |||
| + | |||
| + | * **March 19th, Wednesday ** (4-5pm) \\ \\ | ||
| + | | ||
| + | | ||
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| + | \\ | ||
| + | <WRAP box 80%> **// | ||
| + | |||
| + | We will then discuss recent works that show how this connection can be exploited to prove new results regarding so-called " | ||
| + | |||
| + | This talk will feature discussions of various joint works with Promit Ghosal, Wilson Li, Yuchen Liao, and Mykhaylo Shkolnikov. | ||
| + | |||
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| + | |||
| + | \\ | ||
| + | </ | ||
| + | \\ \\ | ||
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| + | |||
| + | |||
| + | * **March 26th, Wednesday ** (4-5pm) \\ \\ | ||
| + | **// | ||
| + | **// | ||
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| + | \\ | ||
| + | <WRAP box 80%> **// | ||
| + | |||
| + | |||
| + | \\ | ||
| + | </ | ||
| + | \\ \\ | ||
| + | |||
| + | |||
| + | * **April 2nd, Wednesday ** (4-5pm) \\ \\ | ||
| + | | ||
| + | \\ | ||
| + | <WRAP box 80%> **// | ||
| + | |||
| + | |||
| + | |||
| + | </ | ||
| + | \\ \\ | ||
| + | |||
| + | |||
| + | |||
| + | * **April 9th, Wednesday ** (4-5pm) | ||
| + | | ||
| + | | ||
| + | |||
| + | \\ | ||
| + | <WRAP box 80%> **// | ||
| + | |||
| + | | ||
| + | \\ | ||
| + | </ | ||
| + | \\ \\ | ||
| + | |||
| + | |||
| + | |||
| + | * **April 16th, Wednesday, 2: | ||
| + | | ||
| + | **// | ||
| + | \\ | ||
| + | <WRAP box 80%> **// | ||
| + | |||
| + | \\ | ||
| + | </ | ||
| + | \\ \\ | ||
| + | |||
| + | * **April 16th, Wednesday ** (4-5pm) ****\\ | ||
| + | | ||
| + | | ||
| + | \\ | ||
| + | <WRAP box 80%> **// | ||
| + | |||
| + | The growing interest in the theory and applications of nonlocal diffusion models naturally raises questions about analogues of Li-Yau-type inequalities in the nonlocal setting. However, despite many parallels between local and nonlocal diffusion models, even the model case of fractional heat flow presents both conceptual and technical challenges. | ||
| + | |||
| + | In my talk, I will discuss recent progress on optimal differential Harnack bounds for fractional heat flow. In particular, I will show how the structural properties of these estimates offer new insights into classical results for the standard heat equation. | ||
| + | |||
| + | \\ | ||
| + | </ | ||
| + | \\ \\ | ||
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| + | |||
| + | * **April 30th, Wednesday ** (4-5pm) \\ \\ | ||
| + | | ||
| + | | ||
| + | \\ | ||
| + | <WRAP box 80%> **// | ||
| + | |||
| + | |||
| + | First, we will develop the theory of pseudodifferential operators on Euclidean space. This involves, for example, proving properties regarding the taking of adjoints, of composing two operators, etc. We will prove the existence of a pseudo-inverse, | ||
| + | |||
| + | |||
| + | No prior knowledge about differential equations or cohomology will be assumed. | ||
| + | |||
| + | |||
| + | \\ | ||
| + | </ | ||
| + | \\ \\ | ||
| + | |||
| + | |||
| + | |||
| + | |||
| + | * **May 7th, Wednesday ** (4-5pm) \\ \\ | ||
| + | | ||
| + | | ||
| + | second-order perturbations | ||
| + | |||
| + | \\ | ||
| + | <WRAP box 80%> **// | ||
| + | solutions to Schroedinger and wave equations, whose Hamiltonian | ||
| + | $H=-\Delta+iA \cdot \nabla + V$ contains a magnetic potential (a | ||
| + | first-order perturbation) or where the Laplacian is replaced by the | ||
| + | Laplace-Beltrami operator on a more general manifold (second-order | ||
| + | perturbations). | ||
| + | |||
| + | \\ | ||
| + | </ | ||
| + | \\ \\ | ||
| + | |||
| + | |||
| + | |||
| + | --------- | ||
| + | |||
| + | |||
| + | |||
| + | |||
| + | |||
| + | |||
| + | --------- | ||
| + | |||
| + | |||
| + | |||
| + | |||
| + | |||
| + | ====Fall 2024==== | ||
| + | |||
| + | |||
| + | |||
| + | |||
| + | * **August 21st, Wednesday ** (3: | ||
| + | **//Speaker //**: \\ | ||
| + | **// | ||
| + | \\ \\ | ||
| + | |||
| + | |||
| + | |||
| + | |||
| + | |||
| + | |||
| + | * **September 18th, Wednesday ** (3: | ||
| + | **//Speaker //**: Ao Sun (Lehigh University) \\ | ||
| + | **// | ||
| + | \\ \\ | ||
| + | <WRAP box 80%> | ||
| + | **// | ||
| + | \\ | ||
| + | </ | ||
| + | \\ \\ | ||
| + | |||
| + | |||
| + | |||
| + | * **October 2nd , Wednesday ** (3: | ||
| + | **// | ||
| + | **// | ||
| + | \\ | ||
| + | <WRAP box 80%> | ||
| + | **// | ||
| + | |||
| + | |||
| + | \\ | ||
| + | </ | ||
| + | \\ \\ | ||
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| + | |||
| + | * **October 23rd, Wednesday ** (3: | ||
| + | **// | ||
| + | **// | ||
| + | \\ | ||
| + | <WRAP box 80%> | ||
| + | **// | ||
| + | We show for a large class of entire functions, $f$, that after proper rescaling, on compact sets, the derivatives of $f$ converge to cosine, in particular their roots become evenly spaced. This proves a conjecture of Farmer and Rhoades [Trans. Amer. Math. Soc., 357(9): | ||
| + | \\ | ||
| + | </ | ||
| + | \\ \\ | ||
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| + | |||
| + | * **October 30th, Wednesday ** (3: | ||
| + | **// | ||
| + | **// | ||
| + | \\ | ||
| + | <WRAP box 80%> | ||
| + | **// | ||
| + | </ | ||
| + | \\ \\ | ||
| + | |||
| + | |||
| + | |||
| + | * **November 27th, Wednesday ** (3: | ||
| + | **// | ||
| + | **// | ||
| + | \\ | ||
| + | <WRAP box 80%> **// | ||
| + | |||
| + | \\ | ||
| + | </ | ||
| + | \\ \\ | ||
| + | |||
| + | |||
| + | |||
| + | |||
| + | * **December 6th, Friday ** (3: | ||
| + | **// | ||
| + | **// | ||
| + | \\ | ||
| + | <WRAP box 80%> **// | ||
| + | |||
| + | \\ | ||
| + | </ | ||
| + | \\ \\ | ||
| + | |||
| + | |||
| + | |||
| + | ---- | ||
| + | |||
| + | |||
| + | ---- | ||
| + | |||
| + | ====Spring 2024==== | ||
| + | |||
| + | |||
| + | |||
| + | |||
| + | * **January 24th, Wednesday ** (4-5pm)\\ | ||
| + | \\ \\ | ||
| + | <WRAP box 80%> **// | ||
| + | \\ | ||
| + | </ | ||
| + | \\ \\ | ||
| + | |||
| + | |||
| + | |||
| + | |||
| + | * ** February 29th, Thursday (Special date) ** (4-5pm) \\ | ||
| + | \\ | ||
| + | **// | ||
| + | |||
| + | \\ \\ | ||
| + | <WRAP box 80%> | ||
| + | **// | ||
| + | |||
| + | $$\widehat{f}(m)=\frac{1}{N} \sum_{x=0}^{N-1} e^{-\frac{2 \pi i xm}{N}} f(x),$$ | ||
| + | |||
| + | and that the values of $\widehat{f}(m), | ||
| + | \\ | ||
| + | </ | ||
| + | \\ \\ | ||
| + | |||
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| + | |||
| + | |||
| + | |||
| + | |||
| + | |||
| + | |||
| + | * **March 6th, Wednesday ** (4-5pm) **(Spring Break)**\\ | ||
| + | \\ | ||
| + | **// | ||
| + | \\ | ||
| + | <WRAP box 80%> **// | ||
| + | \\ | ||
| + | </ | ||
| + | \\ \\ | ||
| + | |||
| + | |||
| + | |||
| + | |||
| + | * **March 13th, Wednesday ** (4-5pm) \\ \\ | ||
| + | | ||
| + | | ||
| + | \\ | ||
| + | <WRAP box 80%> | ||
| + | **// | ||
| + | Muskat problem. We show the global existence of weak solutions to the model. We then present a high-order accurate bound-preserving and unconditionally stable numerical method for solving the equations. The talk is based on works joint with Yali Gao and Xiaoming Wang. | ||
| + | |||
| + | \\ | ||
| + | </ | ||
| + | \\ \\ | ||
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| + | |||
| + | * **March 20th, Wednesday ** (4-5pm) \\ \\ | ||
| + | | ||
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| + | \\ | ||
| + | <WRAP box 80%> **// | ||
| + | |||
| + | |||
| + | \\ | ||
| + | </ | ||
| + | \\ \\ | ||
| + | |||
| + | |||
| + | |||
| + | |||
| + | * **April 17th, Wednesday ** (4-5pm) \\ \\ | ||
| + | | ||
| + | **// | ||
| + | \\ | ||
| + | <WRAP box 80%> **// | ||
| + | |||
| + | |||
| + | |||
| + | This is joint work with Xiaoqi Huang following earlier work with Matthew Blair. | ||
| + | |||
| + | About the Speaker: | ||
| + | |||
| + | \\ | ||
| + | </ | ||
| + | \\ \\ | ||
| + | |||
| + | |||
| + | * **April 24th, Wednesday ** (4-5pm) **(Passover Break)**\\ | ||
| + | | ||
| + | | ||
| + | \\ | ||
| + | <WRAP box 80%> **// | ||
| + | |||
| + | \\ | ||
| + | </ | ||
| + | \\ \\ | ||
| + | |||
| + | |||
| + | |||
| + | * **May 1st, Wednesday ** (4-5pm) \\ \\ | ||
| + | | ||
| + | | ||
| + | \\ | ||
| + | <WRAP box 80%> **// | ||
| + | |||
| + | |||
| + | \\ | ||
| + | </ | ||
| + | \\ \\ | ||
| + | |||
| + | |||
| + | |||
| + | |||
| + | |||
| + | |||
| + | |||
| + | --------- | ||
| + | |||
| + | |||
| + | |||
| + | |||
| + | |||
| + | ====Fall 2023==== | ||
| + | |||
| + | |||
| + | |||
| + | |||
| + | * **August 23rd, Wednesday ** (3: | ||
| + | **//Speaker //**: \\ | ||
| + | **// | ||
| + | \\ \\ | ||
| + | |||
| + | |||
| + | |||
| + | |||
| + | * **August 30th, Wednesday ** (3: | ||
| + | **//Speaker //**: Emmett Wyman (Binghamton University) \\ | ||
| + | **// | ||
| + | <WRAP box 80%> | ||
| + | **// | ||
| + | When you hit a drum, the sound it makes is a mix of overtones with frequencies corresponding to the drum's Laplace eigenvalues. A classic paper by Kac ["Can one hear the shape of a drum?" 1966] asks if the frequencies of these overtones uniquely determine the shape of the drum head. This question is still richly studied. | ||
| + | |||
| + | Yakun Xi and I recently posed a related question: Can one hear where a drum is struck? Imagine you know a drum's shape. Could you determine where it is struck, up to symmetry, by listening also to the amplitudes of these overtones? | ||
| + | |||
| + | In this talk, I will state this problem precisely, give additional physical interpretations, | ||
| + | \\ | ||
| + | </ | ||
| + | \\ \\ | ||
| + | |||
| + | |||
| + | |||
| + | |||
| + | * **September 13th, Wednesday ** (3: | ||
| + | **// Speaker //**: Zongyuan Li (Binghamton University) \\ | ||
| + | **// | ||
| + | \\ \\ | ||
| + | <WRAP box 80%> | ||
| + | **// | ||
| + | |||
| + | \\ | ||
| + | </ | ||
| + | \\ \\ | ||
| + | |||
| + | |||
| + | * **September 20th, Wednesday ** (3: | ||
| + | **//Speaker //**: Xiangjin Xu (Binghamton University) \\ | ||
| + | **// | ||
| + | \\ \\ | ||
| + | <WRAP box 80%> | ||
| + | **// | ||
| + | |||
| + | In this talk, on a complete Riemannian manifold $(M,g)$ with $Ric(M)\geq 0$, I will discuss my recent work on the sharp estimates of the heat kernel and Green' | ||
| + | \\ | ||
| + | </ | ||
| + | \\ \\ | ||
| + | |||
| + | |||
| + | |||
| + | * **October 4th , Wednesday ** (3: | ||
| + | **// | ||
| + | **// | ||
| + | \\ | ||
| + | <WRAP box 80%> | ||
| + | **// | ||
| + | |||
| + | |||
| + | \\ | ||
| + | </ | ||
| + | \\ \\ | ||
| + | |||
| + | |||
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| + | |||
| + | |||
| + | |||
| + | * **October 18th, Wednesday ** (3: | ||
| + | **// | ||
| + | **// | ||
| + | \\ | ||
| + | <WRAP box 80%> | ||
| + | **// | ||
| + | |||
| + | \\ | ||
| + | </ | ||
| + | \\ \\ | ||
| + | |||
| + | |||
| + | |||
| + | |||
| + | |||
| + | |||
| + | * **November 22nd, Wednesday ** (3: | ||
| + | **// | ||
| + | **// | ||
| + | \\ | ||
| + | <WRAP box 80%> | ||
| + | **// | ||
| + | \\ | ||
| + | </ | ||
| + | \\ \\ | ||
| + | |||
| + | |||
| + | ------------ | ||
| + | |||
| + | |||
| + | ====Spring 2023==== | ||
| + | |||
| + | |||
| + | |||
| + | |||
| + | * **January 25th, Wednesday ** (3: | ||
| + | \\ \\ | ||
| + | <WRAP box 80%> **// | ||
| + | \\ | ||
| + | </ | ||
| + | \\ \\ | ||
| + | |||
| + | |||
| + | |||
| + | |||
| + | |||
| + | |||
| + | * ** February 22nd, Wednesday ** (3: | ||
| + | \\ | ||
| + | \\ \\ | ||
| + | for a nonlinear heat equation | ||
| + | |||
| + | \\ \\ | ||
| + | <WRAP box 80%> **// | ||
| + | semester, in this talk I will discuss some improved estimates for the | ||
| + | behavior of generic singularities for solutions of the equation | ||
| + | $\partial_{\tau} u = \partial_y^2 u +u^3$. Studying the dynamics of | ||
| + | nonlinear heat equations such as this one have proven very fruitful in | ||
| + | studying the singularities of PDEs arising from geometric flows, | ||
| + | including mean curvature flow and Ricci flow. | ||
| + | |||
| + | Because of the cubic nonlinearity, | ||
| + | in finite time. In the previous talk, the generic blowup dynamics was | ||
| + | discussed in terms of the rescaled solution $v(y,\tau) = \sqrt{T-t} | ||
| + | u(x,t)$, where $y:= x / \sqrt{T-t}$, | ||
| + | the blowup time of $u$. Ideally, we would like to use the dynamics of | ||
| + | this rescaled solution to study the original, however, the spacetime | ||
| + | region the previous results were considered in is too small to be of | ||
| + | much use. We discuss this issue in more detail, along with some | ||
| + | techniques used to expand the region of effective control. | ||
| + | \\ | ||
| + | </ | ||
| + | \\ \\ | ||
| + | |||
| + | |||
| + | |||
| + | |||
| + | * **March 2nd, Thursday ** (3: | ||
| + | | ||
| + | **// | ||
| + | \\ | ||
| + | <WRAP box 80%> **// | ||
| + | |||
| + | \\ | ||
| + | </ | ||
| + | \\ \\ | ||
| + | |||
| + | |||
| + | |||
| + | |||
| + | |||
| + | |||
| + | * **March 22nd, Wednesday ** (3: | ||
| + | \\ | ||
| + | \\ **// | ||
| + | \\ | ||
| + | <WRAP box 80%> **// | ||
| + | |||
| + | \\ | ||
| + | </ | ||
| + | \\ \\ | ||
| + | |||
| + | |||
| + | |||
| + | * **March 29th, Wednesday ** (3: | ||
| + | \\ | ||
| + | \\ | ||
| + | |||
| + | |||
| + | \\ | ||
| + | <WRAP box 80%> **// | ||
| + | |||
| + | \\ | ||
| + | </ | ||
| + | \\ \\ | ||
| + | |||
| + | |||
| + | * **April 5th, Wednesday ** (3: | ||
| + | \\ | ||
| + | \\ **// | ||
| + | \\ | ||
| + | <WRAP box 80%> **// | ||
| + | |||
| + | |||
| + | |||
| + | </ | ||
| + | \\ \\ | ||
| + | |||
| + | |||
| + | |||
| + | * **April 12th, Wednesday ** (3: | ||
| + | \\ | ||
| + | \\ | ||
| + | \\ | ||
| + | <WRAP box 80%> **// | ||
| + | |||
| + | | ||
| + | \\ | ||
| + | </ | ||
| + | \\ \\ | ||
| + | |||
| + | |||
| + | |||
| + | |||
| + | |||
| + | * **April 26th, Wednesday ** (3: | ||
| + | \\ | ||
| + | \\ **// | ||
| + | \\ | ||
| + | <WRAP box 80%> **// | ||
| + | |||
| + | \\ | ||
| + | </ | ||
| + | \\ \\ | ||
| + | |||
| + | |||
| + | |||
| + | |||
| + | |||
| + | --------- | ||
| + | |||
| + | |||
| + | |||
| + | ====Fall 2022==== | ||
| + | |||
| + | |||
| + | |||
| + | |||
| + | * **September 7th, Wednesday ** (3: | ||
| + | **//Speaker //**: \\ | ||
| + | **// | ||
| + | \\ \\ | ||
| + | |||
| + | |||
| + | |||
| + | |||
| + | |||
| + | * **September 21st, Wednesday ** (3: | ||
| + | **//Speaker //**: Xiangjin Xu (Binghamton University) \\ | ||
| + | **// | ||
| + | \\ \\ | ||
| + | <WRAP box 80%> | ||
| + | **// | ||
| + | |||
| + | \\ | ||
| + | </ | ||
| + | \\ \\ | ||
| + | |||
| + | |||
| + | |||
| + | * **September 28th, Wednesday ** (3: | ||
| + | **// Speaker //**: Gang Zhou (Binghamton University)\\ | ||
| + | **// | ||
| + | continuity of Ising model’s spontaneous magnetization" | ||
| + | \\ \\ | ||
| + | <WRAP box 80%> | ||
| + | **// | ||
| + | continuity of Ising model’s spontaneous magnetization" | ||
| + | |||
| + | In the paper they considered three dimensional antiferromagnetic Ising model. It is known that at the high temperature, | ||
| + | |||
| + | A crucial technique is the so-called switching lemma. It establishes a bijection between undirected graphs generated by the random current representation. In many important papers this was used, including the ones helping Hugo Duminil-Copin to win a Fields medal in 2022. | ||
| + | |||
| + | However this technique does not work for the other spin models, for example, XY model or most of the quantum models. | ||
| + | |||
| + | Any input is welcome. | ||
| + | |||
| + | \\ | ||
| + | </ | ||
| + | \\ \\ | ||
| + | |||
| + | |||
| + | |||
| + | * **October 5th , Wednesday ** (3: | ||
| + | **// | ||
| + | **// | ||
| + | \\ | ||
| + | <WRAP box 80%> | ||
| + | **// | ||
| + | |||
| + | |||
| + | \\ | ||
| + | </ | ||
| + | \\ \\ | ||
| + | |||
| + | |||
| + | |||
| + | * **October 12th, Wednesday ** (3: | ||
| + | **// | ||
| + | **// | ||
| + | \\ \\ | ||
| + | <WRAP box 80%> | ||
| + | **// | ||
| + | |||
| + | \\ | ||
| + | </ | ||
| + | \\ \\ | ||
| + | |||
| + | |||
| + | |||
| + | |||
| + | * **October 19th, Wednesday ** (3: | ||
| + | **// | ||
| + | **// | ||
| + | \\ | ||
| + | <WRAP box 80%> | ||
| + | **// | ||
| + | |||
| + | \\ | ||
| + | </ | ||
| + | \\ \\ | ||
| + | |||
| + | |||
| + | |||
| + | |||
| + | |||
| + | |||
| + | * **October 26th, Wednesday ** (3: | ||
| + | **// | ||
| + | **// | ||
| + | \\ | ||
| + | <WRAP box 80%> | ||
| + | **// | ||
| + | Self-similar Blow-up of Semilinear Heat Equations" | ||
| + | and Robert V. Kohn, and " | ||
| + | $u_t-\Delta u = u^p$" by Stathis Filippas and Robert V. Kohn. The | ||
| + | authors study the blowup dynamics of semilinear heat equation | ||
| + | $u_t-\Delta u = u^p, p>1$ in $\mathbb{R}^n$ in both papers, with the first | ||
| + | paving the way for the second. This nonlinear heat equation has | ||
| + | structure similar to many other nonlinear equations, in particular | ||
| + | several which arise in geometric analysis, and so often the techniques | ||
| + | used to study the dynamics of spacial blow up of this equation may be | ||
| + | used to study the blowup of curvature in geometric flows. | ||
| + | |||
| + | Giga and Kohn show that for blowup solutions u which satisfy a weak | ||
| + | blowup growth restriction, | ||
| + | approaches its steady state solution asymptotically. Fillipas and Kohn | ||
| + | then study the long time behavior of the rescaled solution from a | ||
| + | dynamical systems point of view: by projecting the equation satisfied | ||
| + | by v onto suitably chosen subspaces, one can show that the long time | ||
| + | behavior is dominated by the neutral mode, whose dynamics may be | ||
| + | obtained exactly. | ||
| + | |||
| + | Some more recent and current work will be briefly discussed at the end. | ||
| + | |||
| + | |||
| + | \\ | ||
| + | </ | ||
| + | \\ \\ | ||
| + | |||
| + | |||
| + | |||
| + | |||
| + | |||
| + | |||
| + | |||
| + | * **November 2nd, Wednesday ** (3: | ||
| + | **// | ||
| + | **// | ||
| + | \\ | ||
| + | <WRAP box 80%> | ||
| + | **// | ||
| + | |||
| + | This is a joint work with Juerg Froehlich. | ||
| + | |||
| + | This is a new direction for me. I will try to answer the questions. | ||
| + | |||
| + | |||
| + | </ | ||
| + | \\ \\ | ||
| + | |||
| + | |||
| + | |||
| + | | ||
| + | **// | ||
| + | **// | ||
| + | |||
| + | \\ | ||
| + | <WRAP box 80%> | ||
| + | **// | ||
| + | |||
| + | | ||
| + | \\ | ||
| + | </ | ||
| + | \\ \\ | ||
| + | |||
| + | |||
| + | |||
| + | |||
| + | * **November 23rd, Wednesday ** (3: | ||
| + | **// | ||
| + | **// | ||
| + | \\ | ||
| + | <WRAP box 80%> | ||
| + | **// | ||
| + | \\ | ||
| + | </ | ||
| + | \\ \\ | ||
| + | |||
| + | |||
| + | ---- | ||
| + | |||
| + | ---- | ||
| + | |||
| + | |||
| + | ====Spring 2020==== | ||
| + | |||
| + | |||
| + | |||
| + | * **January 22nd, Wednesday ** (4: | ||
| + | \\ \\ | ||
| + | |||
| + | * **January 29th, Wednesday ** (4: | ||
| + | \\ | ||
| + | \\ **// | ||
| + | \\ \\ | ||
| + | <WRAP box 80%> **// | ||
| + | \\ | ||
| + | </ | ||
| + | \\ \\ | ||
| + | |||
| + | |||
| + | |||
| + | * **February 5th, Wednesday ** (4: | ||
| + | \\ | ||
| + | \\ **// | ||
| + | \\ \\ | ||
| + | <WRAP box 80%> **// | ||
| + | |||
| + | \\ | ||
| + | </ | ||
| + | \\ \\ | ||
| + | |||
| + | |||
| + | |||
| + | * **February 12th, Wednesday ** (3: | ||
| + | \\ **// Speaker //**: Guillaume Dubach (CUNY Baruch) | ||
| + | \\ **// | ||
| + | \\ \\ | ||
| + | <WRAP box 80%> **// | ||
| + | \\ | ||
| + | </ | ||
| + | \\ \\ | ||
| + | |||
| + | |||
| + | |||
| + | * **February 19th , Wednesday ** (3: | ||
| + | \\ | ||
| + | \\ **// | ||
| + | \\ | ||
| + | <WRAP box 80%> **// | ||
| + | |||
| + | \\ | ||
| + | </ | ||
| + | \\ \\ | ||
| + | |||
| + | |||
| + | |||
| + | * ** February 26th , Wednesday ** (4: | ||
| + | \\ | ||
| + | \\ | ||
| + | \\ \\ | ||
| + | <WRAP box 80%> **// | ||
| + | |||
| + | \\ | ||
| + | </ | ||
| + | \\ \\ | ||
| + | |||
| + | |||
| + | |||
| + | |||
| + | * **March 4th, Wednesday ** (4: | ||
| + | \\ | ||
| + | \\ **// | ||
| + | \\ | ||
| + | <WRAP box 80%> **// | ||
| + | |||
| + | \\ | ||
| + | </ | ||
| + | \\ \\ | ||
| + | |||
| + | |||
| + | |||
| + | |||
| + | |||
| + | * **March 18th, Wednesday ** (4: | ||
| + | \\ | ||
| + | \\ **// | ||
| + | \\ | ||
| + | <WRAP box 80%> **// | ||
| + | |||
| + | \\ | ||
| + | </ | ||
| + | \\ \\ | ||
| + | |||
| + | |||
| + | |||
| + | |||
| + | * **March 25th, Wednesday ** (4: | ||
| + | \\ | ||
| + | \\ **// | ||
| + | \\ | ||
| + | <WRAP box 80%> **// | ||
| + | |||
| + | \\ | ||
| + | </ | ||
| + | \\ \\ | ||
| + | |||
| + | |||
| + | |||
| + | |||
| + | * **April 1st, Wednesday ** (4: | ||
| + | \\ | ||
| + | \\ **// | ||
| + | \\ | ||
| + | <WRAP box 80%> **// | ||
| + | |||
| + | </ | ||
| + | \\ \\ | ||
| + | |||
| + | |||
| + | |||
| + | * **April 8th, Wednesday ** (4: | ||
| + | \\ | ||
| + | \\ **// | ||
| + | \\ | ||
| + | <WRAP box 80%> **// | ||
| + | | ||
| + | \\ | ||
| + | </ | ||
| + | \\ \\ | ||
| + | |||
| + | |||
| + | |||
| + | * **April 15th, Wednesday ** (4: | ||
| + | \\ | ||
| + | <WRAP box 80%> **// | ||
| + | |||
| + | \\ | ||
| + | </ | ||
| + | \\ \\ | ||
| + | |||
| + | |||
| + | * **April 22nd, Wednesday ** (4: | ||
| + | \\ | ||
| + | \\ **// | ||
| + | \\ | ||
| + | <WRAP box 80%> **// | ||
| + | |||
| + | \\ | ||
| + | </ | ||
| + | \\ \\ | ||
| + | |||
| + | |||
| + | --------- | ||
| + | |||
| + | |||
| + | ====Fall 2019==== | ||
| + | |||
| + | |||
| + | |||
| + | |||
| + | * **August 28th, Wednesday ** (3: | ||
| + | \\ | ||
| + | \\ **// | ||
| + | \\ \\ | ||
| + | |||
| + | * **September 4th, Wednesday ** (3: | ||
| + | \\ \\ | ||
| + | <WRAP box 80%> **// | ||
| + | \\ | ||
| + | </ | ||
| + | \\ \\ | ||
| + | |||
| + | |||
| + | |||
| + | * **September 5th, Thursday ** (WH 309, 2: | ||
| + | \\ | ||
| + | \\ **// | ||
| + | \\ \\ | ||
| + | <WRAP box 80%> **// | ||
| + | </ | ||
| + | \\ \\ | ||
| + | |||
| + | |||
| + | |||
| + | |||
| + | * **September 18th, Wednesday ** (4: | ||
| + | \\ **// Speaker //**: Xiangjin Xu (Binghamton University) | ||
| + | \\ **// | ||
| + | \\ \\ | ||
| + | <WRAP box 80%> **// | ||
| + | |||
| + | \\ | ||
| + | </ | ||
| + | \\ \\ | ||
| + | |||
| + | |||
| + | |||
| + | * **September 25th , Wednesday ** (3: | ||
| + | \\ | ||
| + | \\ **// | ||
| + | \\ | ||
| + | <WRAP box 80%> **// | ||
| + | |||
| + | |||
| + | |||
| + | \\ | ||
| + | </ | ||
| + | \\ \\ | ||
| + | |||
| + | |||
| + | |||
| + | |||
| + | |||
| + | |||
| + | * **October 9th, Wednesday ** (3: | ||
| + | \\ | ||
| + | \\ **// | ||
| + | \\ | ||
| + | <WRAP box 80%> **// | ||
| + | |||
| + | \\ | ||
| + | </ | ||
| + | \\ \\ | ||
| + | |||
| + | |||
| + | |||
| + | |||
| + | * **October 17th, Thursday ** (1: | ||
| + | \\ | ||
| + | \\ **// | ||
| + | \\ | ||
| + | <WRAP box 80%> **// | ||
| + | \\ | ||
| + | </ | ||
| + | \\ \\ | ||
| + | |||
| + | |||
| + | |||
| + | |||
| + | * **October 23rd, Wednesday ** (4: | ||
| + | \\ | ||
| + | \\ **// | ||
| + | \\ | ||
| + | <WRAP box 80%> **// | ||
| + | Although most of the evidence says the universe is flat, it need not imply the universe looks like $R^3$. | ||
| + | In this talk we discuss the most plausible candidates for the shape of the universe and how to go about detecting such models. | ||
| + | |||
| + | \\ | ||
| + | </ | ||
| + | \\ \\ | ||
| + | |||
| + | |||
| + | |||
| + | |||
| + | |||
| + | |||
| + | * **November 6th, Wednesday ** (4: | ||
| + | \\ | ||
| + | \\ **// | ||
| + | \\ | ||
| + | <WRAP box 80%> **// | ||
| + | |||
| + | </ | ||
| + | \\ \\ | ||
| + | |||
| + | |||
| + | |||
| + | * **November 13th, Wednesday ** (4: | ||
| + | \\ | ||
| + | \\ **// | ||
| + | \\ | ||
| + | <WRAP box 80%> **// | ||
| + | | ||
| + | \\ | ||
| + | </ | ||
| + | \\ \\ | ||
| + | |||
| + | |||
| + | |||
| + | * **November 27th, Wednesday ** (3: | ||
| + | \\ | ||
| + | \\ **// | ||
| + | \\ | ||
| + | <WRAP box 80%> **// | ||
| + | \\ | ||
| + | </ | ||
| + | \\ \\ | ||
| + | |||
| + | |||
| + | |||
| + | * **December 6th, Friday ** (2: | ||
| + | **// | ||
| + | **// | ||
| + | |||
| + | \\ | ||
| + | <WRAP box 80%> **// | ||
| + | |||
| + | \\ | ||
| + | </ | ||
| + | \\ \\ | ||
| + | |||
| + | | ||
| + | \\ \\ | ||
| + | |||
| + | ---- | ||
| + | |||
| + | |||
| + | |||
| + | ====Spring 2019==== | ||
| + | |||
| + | |||
| + | |||
| + | * **January 23rd, Wednesday ** (3: | ||
| + | \\ | ||
| + | \\ **// | ||
| + | \\ \\ | ||
| + | |||
| + | * **January 30th, Wednesday ** (3: | ||
| + | \\ | ||
| + | \\ **// | ||
| + | \\ \\ | ||
| + | <WRAP box 80%> **// | ||
| + | \\ | ||
| + | </ | ||
| + | \\ \\ | ||
| + | |||
| + | |||
| + | |||
| + | |||
| + | |||
| + | * **May 1st, Wednesday ** (3: | ||
| + | \\ | ||
| + | \\ **// | ||
| + | |||
| + | \\ | ||
| + | <WRAP box 80%> **// | ||
| + | |||
| + | \\ | ||
| + | </ | ||
| + | \\ \\ | ||
| + | |||
| + | |||
| + | |||
| + | |||
| + | * **May 8th, Wednesday ** (3: | ||
| + | \\ | ||
| + | \\ **// | ||
| + | \\ | ||
| + | <WRAP box 80%> **// | ||
| + | We discuss uniqueness for mean curvature flow of non-compact manifolds. We use an energy argument to prove a uniqueness theorem for mean curvature flow with possibly unbounded curvatures. These generalize the results in Chen and Yin (CAG, 07). This is a joint work with Man-Chun Lee. | ||
| + | |||
| + | \\ | ||
| + | </ | ||
| + | \\ \\ | ||
| + | |||
| + | |||
| + | |||
| + | ---- | ||
| + | |||
| + | ====Fall 2018==== | ||
| + | |||
| + | |||
| + | |||
| + | * **August 29th, Wednesday ** (3: | ||
| + | \\ | ||
| + | \\ **// | ||
| + | \\ \\ | ||
| + | |||
| + | * **September 5th, Wednesday ** (3: | ||
| + | \\ | ||
| + | \\ **// | ||
| + | \\ \\ | ||
| + | <WRAP box 80%> **// | ||
| + | \\ | ||
| + | </ | ||
| + | \\ \\ | ||
| + | |||
| + | |||
| + | |||
| + | * **September 12th, Wednesday ** (3: | ||
| + | \\ | ||
| + | \\ **// | ||
| + | \\ \\ | ||
| + | <WRAP box 80%> **// | ||
| + | |||
| + | \\ | ||
| + | </ | ||
| + | \\ \\ | ||
| + | |||
| + | |||
| + | |||
| + | * **September 19th, Wednesday ** (3: | ||
| + | | ||
| + | \\ **// | ||
| + | \\ \\ | ||
| + | <WRAP box 80%> **// | ||
| + | \\ | ||
| + | </ | ||
| + | \\ \\ | ||
| + | |||
| + | |||
| + | |||
| + | * **September 26th , Wednesday ** (3: | ||
| + | \\ | ||
| + | \\ **// | ||
| + | \\ | ||
| + | <WRAP box 80%> **// | ||
| + | However, solving the heat equation explicitly and extracting the geometric | ||
| + | information can be difficulty. In this talk, I will offer a new approach | ||
| + | to the heat equation using planar diagrams. The heat kernel constructed | ||
| + | will not be the authentic heat kernel for the surface, but we will show | ||
| + | how it captures geometry. | ||
| + | |||
| + | |||
| + | |||
| + | \\ | ||
| + | </ | ||
| + | \\ \\ | ||
| + | |||
| + | |||
| + | |||
| + | * **October 3rd, Wednesday ** (3: | ||
| + | \\ | ||
| + | \\ | ||
| + | \\ \\ | ||
| + | <WRAP box 80%> **// | ||
| + | |||
| + | \\ | ||
| + | </ | ||
| + | \\ \\ | ||
| + | |||
| + | |||
| + | |||
| + | |||
| + | |||
| + | * **October 17th, Wednesday ** (3: | ||
| + | \\ | ||
| + | \\ **// | ||
| + | \\ | ||
| + | <WRAP box 80%> **// | ||
| + | \\ | ||
| + | </ | ||
| + | \\ \\ | ||
| + | |||
| + | |||
| + | |||
| + | |||
| + | * **October 24th, Wednesday ** (3: | ||
| + | \\ | ||
| + | \\ **// | ||
| + | \\ | ||
| + | <WRAP box 80%> **// | ||
| + | |||
| + | \\ | ||
| + | </ | ||
| + | \\ \\ | ||
| + | |||
| + | |||
| + | |||
| + | |||
| + | * **October 31st, Wednesday ** (3: | ||
| + | \\ | ||
| + | \\ **// | ||
| + | \\ | ||
| + | <WRAP box 80%> **// | ||
| + | both in local and global version, for the positive solution $u(x,t)$ of the heat equations | ||
| + | $$\partial_t u−\Delta u=0$$ | ||
| + | on a complete manifold with $Ric(M)\geq −k$. As applications, | ||
| + | |||
| + | \\ | ||
| + | </ | ||
| + | \\ \\ | ||
| + | |||
| + | |||
| + | |||
| + | * **November 14th, Wednesday ** (3: | ||
| + | \\ | ||
| + | \\ **// | ||
| + | to Random Matrix Theory | ||
| + | \\ | ||
| + | <WRAP box 80%> **// | ||
| + | Matrix Theory allow for a precise | ||
| + | description of the fluctuations of single eigenvalues in the spectrum of | ||
| + | large symmetric matrices. No prior | ||
| + | knowledge of random matrix theory will be assumed. | ||
| + | |||
| + | (Based on joint work with B Landon and HT Yau). | ||
| + | | ||
| + | \\ | ||
| + | </ | ||
| + | \\ \\ | ||
| + | |||
| + | |||
| + | |||
| + | * **November 21st, Wednesday ** (3: | ||
| + | \\ | ||
| + | \\ **// | ||
| + | \\ | ||
| + | <WRAP box 80%> **// | ||
| + | |||
| + | \\ | ||
| + | </ | ||
| + | \\ \\ | ||
| + | |||
| + | |||
| + | * **November 28th, Wednesday ** (3: | ||
| + | \\ | ||
| + | \\ **// | ||
| + | \\ | ||
| + | <WRAP box 80%> **// | ||
| + | |||
| + | \\ | ||
| + | </ | ||
| + | \\ \\ | ||
| + | |||
| + | |||
| + | |||
| + | * **December 5th, Wednesday ** (3: | ||
| + | \\ | ||
| + | \\ **// | ||
| + | |||
| + | \\ | ||
| + | <WRAP box 80%> **// | ||
| + | |||
| + | \\ | ||
| + | </ | ||
| + | \\ \\ | ||
| + | |||
| + | |||
| + | |||
| + | |||
| + | |||
| + | |||
| + | ---- | ||
| + | |||
| + | ====Spring 2018==== | ||
| + | |||
| + | |||
| + | |||
| + | * **January 17th, Wednesday ** (3: | ||
| + | \\ \\ | ||
| + | |||
| + | * **January 24th, Wednesday ** (3: | ||
| + | \\ \\ | ||
| + | <WRAP box 80%> **// | ||
| + | \\ | ||
| + | </ | ||
| + | \\ \\ | ||
| + | |||
| + | |||
| + | |||
| + | * **January 31st, Wednesday ** (3: | ||
| + | \\ \\ | ||
| + | <WRAP box 80%> **// | ||
| + | surfaces. | ||
| + | \\ | ||
| + | </ | ||
| + | \\ \\ | ||
| + | |||
| + | |||
| + | |||
| + | * **February 7th, Wednesday ** (3: | ||
| + | \\ \\ | ||
| + | <WRAP box 80%> **// | ||
| + | surfaces. | ||
| + | \\ | ||
| + | </ | ||
| + | \\ \\ | ||
| + | |||
| + | |||
| + | |||
| + | * **February 14th , Wednesday ** (3: | ||
| + | \\ | ||
| + | <WRAP box 80%> **// | ||
| + | \\ | ||
| + | </ | ||
| + | \\ \\ | ||
| + | |||
| + | |||
| + | |||
| + | * **February 21st, Wednesday ** (3: | ||
| + | \\ \\ | ||
| + | <WRAP box 80%> **// | ||
| + | \\ | ||
| + | </ | ||
| + | \\ \\ | ||
| + | |||
| + | |||
| + | |||
| + | |||
| + | * **February 28th, Wednesday ** (3: | ||
| + | \\ | ||
| + | <WRAP box 80%> **// | ||
| + | \\ | ||
| + | </ | ||
| + | \\ \\ | ||
| + | |||
| + | |||
| + | |||
| + | |||
| + | * **March 7th, Wednesday ** (3: | ||
| + | \\ | ||
| + | <WRAP box 80%> **// | ||
| + | \\ | ||
| + | </ | ||
| + | \\ \\ | ||
| + | |||
| + | |||
| + | |||
| + | |||
| + | * **March 14th, Wednesday ** (3: | ||
| + | \\ | ||
| + | <WRAP box 80%> **// | ||
| + | \\ | ||
| + | </ | ||
| + | \\ \\ | ||
| + | |||
| + | |||
| + | |||
| + | |||
| + | * **March 21th, Wednesday ** (3: | ||
| + | \\ | ||
| + | <WRAP box 80%> **// | ||
| + | \\ | ||
| + | </ | ||
| + | \\ \\ | ||
| + | |||
| + | |||
| + | |||
| + | |||
| + | * **March 28th, Wednesday ** (3: | ||
| + | \\ | ||
| + | <WRAP box 80%> **// | ||
| + | </ | ||
| + | \\ \\ | ||
| + | |||
| + | |||
| + | |||
| + | * **April 4th, Wednesday ** (3: | ||
| + | \\ | ||
| + | <WRAP box 80%> **// | ||
| + | | ||
| + | \\ | ||
| + | </ | ||
| + | \\ \\ | ||
| + | |||
| + | |||
| + | |||
| + | * **April 11th, Wednesday ** (3: | ||
| + | \\ | ||
| + | <WRAP box 80%> **// | ||
| + | \\ | ||
| + | </ | ||
| + | \\ \\ | ||
| + | |||
| + | |||
| + | * **April 18th, Wednesday ** (3: | ||
| + | \\ | ||
| + | <WRAP box 80%> **// | ||
| + | \\ | ||
| + | </ | ||
| + | \\ \\ | ||
| + | |||
| + | |||
| + | * **April 24th, Tuesday ** (2: | ||
| + | \\ | ||
| + | <WRAP box 80%> **// | ||
| + | \\ | ||
| + | </ | ||
| + | \\ \\ | ||
| + | |||
| + | * **April 25th, Wednesday ** (3: | ||
| + | \\ | ||
| + | <WRAP box 80%> **// | ||
| + | \\ | ||
| + | </ | ||
| + | \\ \\ | ||
| + | |||
| + | |||
| + | |||
| + | * **May 2nd, Wednesday ** (3: | ||
| + | \\ | ||
| + | <WRAP box 80%> **// | ||
| + | \\ | ||
| + | </ | ||
| + | \\ \\ | ||
| + | |||
| + | |||
| + | |||
| + | |||
| + | |||
| + | |||
| + | |||
| + | |||
| + | |||
| + | ====Fall 2017==== | ||
| + | |||
| + | |||
| + | |||
| + | * **August 23th, Wednesday ** (3: | ||
| + | \\ \\ | ||
| + | |||
| + | * **August 30th, Wednesday ** (3: | ||
| + | \\ \\ | ||
| + | <WRAP box 80%> **// | ||
| + | when the boundary of the region is smooth. We will use geometric | ||
| + | techniques to construct an integral operator which gives the solution of | ||
| + | the dirichlet problem when the boundary has corners. | ||
| + | \\ | ||
| + | </ | ||
| + | \\ \\ | ||
| + | |||
| + | |||
| + | |||
| + | * **September 6th, Wednesday ** (3: | ||
| + | \\ \\ | ||
| + | <WRAP box 80%> **// | ||
| + | when the boundary of the region is smooth. We will use geometric | ||
| + | techniques to construct an integral operator which gives the solution of | ||
| + | the dirichlet problem when the boundary has corners. | ||
| + | \\ | ||
| + | </ | ||
| + | \\ \\ | ||
| + | |||
| + | |||
| + | |||
| + | * **September 13th, Wednesday ** (3: | ||
| + | \\ \\ | ||
| + | <WRAP box 80%> **// | ||
| + | \\ | ||
| + | </ | ||
| + | \\ \\ | ||
| + | |||
| + | |||
| + | |||
| + | * **September 20th, Wednesday ** (3: | ||
| + | \\ | ||
| + | <WRAP box 80%> **// | ||
| + | when the boundary of the region is smooth. We will use geometric | ||
| + | techniques to construct an integral operator which gives the solution of | ||
| + | the dirichlet problem when the boundary has corners. | ||
| + | \\ | ||
| + | </ | ||
| + | \\ \\ | ||
| + | |||
| + | |||
| + | |||
| + | * **September 27th, Wednesday ** (3: | ||
| + | \\ \\ | ||
| + | <WRAP box 80%> **// | ||
| + | \\ | ||
| + | </ | ||
| + | \\ \\ | ||
| + | |||
| + | |||
| + | |||
| + | |||
| + | * **October 4th, Wednesday ** (3: | ||
| + | \\ | ||
| + | <WRAP box 80%> **// | ||
| + | \\ | ||
| + | </ | ||
| + | \\ \\ | ||
| + | |||
| + | |||
| + | |||
| + | |||
| + | * **October 11th, Wednesday ** (3: | ||
| + | \\ | ||
| + | <WRAP box 80%> **// | ||
| + | extended to the cases involving product kernels and general multi-parameter setting by B. Street and Stein. | ||
| + | \\ | ||
| + | </ | ||
| + | \\ \\ | ||
| + | |||
| + | |||
| + | |||
| + | |||
| + | * **October 18th, Wednesday ** (3: | ||
| + | \\ | ||
| + | <WRAP box 80%> **// | ||
| + | \\ | ||
| + | </ | ||
| + | \\ \\ | ||
| + | |||
| + | |||
| + | |||
| + | |||
| + | * **October 25th, Wednesday ** (3: | ||
| + | \\ | ||
| + | <WRAP box 80%> **// | ||
| + | \\ | ||
| + | </ | ||
| + | \\ \\ | ||
| + | |||
| + | |||
| + | |||
| + | |||
| + | * **November 1st, Wednesday ** (3: | ||
| + | \\ | ||
| + | <WRAP box 80%> **// | ||
| + | </ | ||
| + | \\ \\ | ||
| + | |||
| + | |||
| + | |||
| + | * **November 8th, Wednesday ** (3: | ||
| + | \\ | ||
| + | <WRAP box 80%> **// | ||
| + | | ||
| + | \\ | ||
| + | </ | ||
| + | \\ \\ | ||
| + | |||
| + | |||
| + | |||
| + | * **November 15th, Wednesday ** (3: | ||
| + | \\ | ||
| + | <WRAP box 80%> **// | ||
| + | \\ | ||
| + | </ | ||
| + | \\ \\ | ||
| + | |||
| + | |||
| + | * **November 22rd, Wednesday ** (Thanksgiving) \\ \\ | ||
| + | \\ | ||
| + | <WRAP box 80%> **// | ||
| + | \\ | ||
| + | </ | ||
| + | \\ \\ | ||
| + | |||
| + | |||
| + | * **November 29th, Wednesday ** (3: | ||
| + | \\ | ||
| + | <WRAP box 80%> **// | ||
| + | For a tuple $A= (A_1; A_2;..... A_n)$ of elements in a unital | ||
| + | |||
| + | A big part of this talk is joint work with R. Grigorchuk. | ||
| + | \\ | ||
| + | </ | ||
| + | \\ \\ | ||
| + | |||
| + | |||
| + | |||
| + | * **December 6th, Wednesday ** (3: | ||
| + | \\ | ||
| + | <WRAP box 80%> **// | ||
| + | values problems for elliptic operators on a compact manifold with boundary. Its properties and applications to address Fredholmness of the operator will be discussed. | ||
| + | \\ | ||
| + | </ | ||
| + | \\ \\ | ||
| + | |||
| + | |||
| + | |||
| + | |||
| + | |||
| + | ====Spring 2017==== | ||
| + | |||
| + | |||
| + | |||
| + | * **January 18th, Wednesday ** (3: | ||
| + | \\ \\ | ||
| + | |||
| + | * **January 25th, Wednesday ** (3: | ||
| + | |||
| + | The lectures are based on the book: **Hangzhou Lectures on Eigenfunctions of the Laplacian, Christopher D. Sogge, (Annals of Mathematics Studies-188), | ||
| + | \\ | ||
| + | </ | ||
| + | \\ \\ | ||
| + | |||
| + | * **February 1st, Wednesday ** (3: | ||
| + | |||
| + | The lectures are based on the book: **Hangzhou Lectures on Eigenfunctions of the Laplacian, Christopher D. Sogge, (Annals of Mathematics Studies-188), | ||
| + | \\ | ||
| + | </ | ||
| + | \\ \\ | ||
| + | |||
| + | * **February 8th, Wednesday ** (3: | ||
| + | \\ | ||
| + | </ | ||
| + | \\ \\ | ||
| + | |||
| + | * **February 15th, Wednesday ** (3: | ||
| + | \\ | ||
| + | **<WRAP box 80%> // | ||
| + | estimates. Moreover, we will see for any point in the domain, | ||
| + | |||
| + | The lectures are based on the book: **Hangzhou Lectures on Eigenfunctions of the Laplacian, Christopher D. Sogge, (Annals of Mathematics Studies-188), | ||
| + | \\ | ||
| + | </ | ||
| + | \\ \\ | ||
| + | |||
| + | * **February 22nd, Wednesday ** (3: | ||
| + | \\ | ||
| + | |||
| + | |||
| + | The lectures are based on the book: **Hangzhou Lectures on Eigenfunctions of the Laplacian, Christopher D. Sogge, (Annals of Mathematics Studies-188), | ||
| + | </ | ||
| + | \\ \\ | ||
| + | |||
| + | * **March 1st, Wednesday ** (3: | ||
| + | |||
| + | |||
| + | The lectures are based on the book: **Hangzhou Lectures on Eigenfunctions of the Laplacian, Christopher D. Sogge, (Annals of Mathematics Studies-188), | ||
| + | \\ | ||
| + | </ | ||
| + | \\ \\ | ||
| + | |||
| + | * **March 8th, Wednesday ** (Winter break) \\ \\ | ||
| + | \\ | ||
| + | </ | ||
| + | \\ \\ | ||
| + | |||
| + | * **March 15th, Wednesday ** (Snow storm) \\ \\ | ||
| + | \\ | ||
| + | </ | ||
| + | \\ \\ | ||
| + | |||
| + | * **March 22nd, Wednesday ** (3: | ||
| + | **<WRAP box 80%> // | ||
| + | \\ | ||
| + | </ | ||
| + | \\ \\ | ||
| + | |||
| + | * **March 29th, Wednesday ** (3: | ||
| + | \\ | ||
| + | investigate it's stationary phase properties. | ||
| + | |||
| + | |||
| + | The lectures will partially base on the book: Hangzhou Lectures on Eigenfunctions of the Laplacian, Christopher D. Sogge, (Annals of Mathematics Studies-188), | ||
| + | |||
| + | \\ | ||
| + | </ | ||
| + | \\ \\ | ||
| + | |||
| + | |||
| + | * **April 5th, Wednesday ** (3: | ||
| + | |||
| + | The lectures will base on the book: Hangzhou Lectures on Eigenfunctions of the Laplacian, Christopher D. Sogge, (Annals of Mathematics Studies-188), | ||
| + | \\ | ||
| + | </ | ||
| + | \\ \\ | ||
| + | |||
| + | * **April 12th, Wednesday ** (Spring break)\\ | ||
| + | \\ | ||
| + | </ | ||
| + | \\ \\ | ||
| + | |||
| + | * **April 19th, Wednesday ** (3: | ||
| + | \\ | ||
| + | </ | ||
| + | \\ \\ | ||
| + | |||
| + | * **April 26th, Wednesday ** (No seminar talk) \\ \\ | ||
| + | \\ | ||
| + | </ | ||
| + | \\ \\ | ||
| + | |||
| + | |||
| + | * **May 3rd, Wednesday ** (3: | ||
| + | Hardy-Sobolev-Maz' | ||
| + | \\ | ||
| + | </ | ||
| + | \\ \\ | ||
| + | |||
| + | |||
| + | * **May 4th, | ||
| + | | ||
| + | |||
| + | This talk is intended to be for the general audience. | ||
| + | \\ | ||
| + | </ | ||
| + | \\ \\ | ||
| + | |||
| + | |||
| + | |||
| + | |||
| + | |||
| + | |||
| + | ====Fall 2016==== | ||
| + | |||
| + | * **September 7th** (3: | ||
| + | \\ \\ | ||
| + | |||
| + | * **September 14th** | ||
| + | |||
| + | \\ \\ | ||
| + | |||
| + | * **September 19th, Monday** | ||
| + | **// | ||
| + | |||
| + | \\ \\ | ||
| + | |||
| + | * **September 28th, Wednesday** | ||
| + | |||
| + | |||
| + | |||
| + | \\ \\ | ||
| + | |||
| + | * **October 5th, Wednesday** | ||
| + | |||
| + | \\ \\ | ||
| + | |||
| + | * **October 12th (Yom Kippur) **\\ \\ | ||
| + | |||
| + | \\ \\ | ||
| + | |||
| + | * **October 19th, Wednesday** | ||
| + | **// | ||
| + | |||
| + | |||
| + | \\ \\ | ||
| + | |||
| + | * **October 26th, Wednesday** | ||
| + | **// | ||
| + | **// | ||
| + | |||
| + | \\ \\ | ||
| + | |||
| + | * **November 2nd**\\ | ||
| + | |||
| + | \\ \\ | ||
| + | |||
| + | * **November 9th**\\ | ||
| + | **// | ||
| + | |||
| + | |||
| + | \\ \\ | ||
| + | |||
| + | * **November 16th**\\ | ||
| + | | ||
| + | |||
| + | \\ \\ | ||
| + | |||
| + | * **November | ||
| + | |||
| + | \\ \\ | ||
| + | |||
| + | * **November 30th, Wednesday** | ||
| + | **// | ||
| + | |||
| + | \\ \\ | ||
| + | |||
| + | * **December 2nd, Friday**(4: | ||
| + | **\\ | ||
| + | <WRAP box 80%> // | ||
| + | Mean curvature flow may be regarded as a geometric version of the heat equation. However, in contrast to the classical heat equation, mean curvature flow is described by a quasilinear evolution system of partial | ||
| + | differential equations, and in general the solution only exists on a finite time interval. Therefore, it's very typical that the flow develops singularities. | ||
| + | |||
| + | Translating solitons arise as parabolic rescaling of type II singularities. In this talk, we shall outline a program on the classification of translating solitons. We shall also report on some recent progress we have made in the joint work with Joel Spruck. \\ | ||
| + | </ | ||
| + | |||
| + | |||
| + | \\ \\ | ||
| + | * **December 5th, Monday**(4: | ||
| + | | ||
| + | <WRAP box 80%> | ||
| + | In this talk I present our recent works, jointly with D.Knopf and I.M.Sigal, on singularity formation under mean curvature flow. By very different techniques, we proved the uniqueness of collapsing cylinder for a generic class of initial surfaces. In the talk some key new elements will be discussed. A few problems, which might be tackled by our techniques, will be formulated.\\ | ||
| + | </ | ||
| + | |||
| + | \\ \\ | ||
| + | * **December 7th, Wednesday**(4: | ||
| + | ** \\ \\ | ||
| + | < | ||
| + | Stochastic heat equation (SHE) with multiplicative noise is an important model. When the diffusion coefficient is linear, this model is also called the parabolic Anderson model, the solution of which traditionally gives the Hopf-Cole solution to the famous KPZ equation. Obtaining various fine properties of its solution will certainly deepen our understanding of these important models. In this talk, I will highlight several interesting properties of SHE and then focus on the probability densities of the solution. | ||
| + | |||
| + | In a recent joint work with Y. Hu and D. Nualart, we establish a necessary and sufficient condition for the existence and regularity of the density of the solution to SHE with measure-valued initial conditions. Under a mild cone condition for the diffusion coefficient, | ||
| + | orders.\\ | ||
| + | </ | ||
| + | |||
| + | \\ \\ | ||
| + | |||
| + | ====Spring 2016==== | ||
| + | |||
| + | * **March 9**\\ \\ | ||
| + | |||
| + | \\ \\ | ||
| + | |||
| + | * **April 13**\\ | ||
| + | |||
| + | \\ \\ | ||
| + | |||
| + | * **April 20**\\ | ||
| + | |||
| + | \\ \\ | ||
| + | |||
| + | |||
| + | |||
| + | * **April 20**\\ | ||
| + | |||
| + | |||
| + | \\ \\ | ||
| + | |||
| + | * **April 27**\\ | ||
| + | |||
| + | \\ \\ | ||
| + | |||
| + | |||
| + | |||
| + | |||
| + | |||
| + | * **May 4**\\ \\ | ||
| + | * \\ \\ | ||
| + | | ||
| + | ====Fall 2015==== | ||
| + | |||
| + | * **October 7**\\ \\ | ||
| + | \\ \\ | ||
| + | |||
| + | |||
| + | |||
| + | * **October 14**\\ | ||
| + | |||
| + | \\ \\ | ||
| + | |||
| + | * **October 22, 2:50-3:50pm (Special Date, Joint with Geometry and Topology Seminar)**\\ | ||
| + | eigenfunctions\\ | ||
| + | \\ \\ | ||
| + | |||
| + | |||
| + | |||
| + | |||
| + | * **October 28**\\ | ||
| + | |||
| + | \\ \\ | ||
| + | |||
| + | |||
| + | * **November 4**\\ \\ | ||
| + | |||
| + | \\ \\ | ||
| + | |||
| + | |||
| + | * **November 18**\\ | ||
| + | |||
| + | \\ \\ | ||
| + | |||
| + | |||
| + | * **December 2**\\ \\ | ||
| + | |||
| + | \\ \\ | ||
| + | |||
| + | |||
| + | |||
| + | |||
| + | |||
| + | |||
| + | |||
| + | |||
| + | |||
| + | ====Spring 2015==== | ||
| + | |||
| + | * **February 26 (unusual day & time: Thursday, 4: | ||
| + | |||
| + | |||
| + | ====Fall 2014==== | ||
| + | |||
| + | * **November 5**\\ \\ | ||
| + | \\ \\ | ||
| + | |||
| + | * **December 3**\\ \\ | ||
| + | \\ \\ | ||
| + | |||
| + | |||
