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Spam yourself with math PhD qualifying-exam questions.

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Stanford Practice, 11 Applied mathematics, total variation denoising, median filtering, fixed-point iteration

Let π‘₯π‘˜, π‘˜=0,1,…,𝑁 be a 1D discretized signal on [0,1]. We assume that the measured signal π‘¦π‘˜ is noisy:

π‘¦π‘˜=π‘₯π‘˜+π‘›π‘˜,

where π‘›π‘˜ is noise. In order to remove the noise, we start an iterative estimation process. Given the iterate π‘₯π‘˜(𝑛) let us define the error estimator

π‘’πœ†(𝑧;π‘₯π‘˜βˆ’1(𝑛),π‘₯π‘˜+1(𝑛),π‘¦π‘˜)=|π‘§βˆ’π‘₯π‘˜βˆ’1(𝑛)|+|π‘§βˆ’π‘₯π‘˜+1(𝑛)|+πœ†|π‘§βˆ’π‘¦π‘˜|,

for π‘§βˆˆβ„. The parameter πœ† regulates how much we weigh the bias toward the initial measurement π‘¦π‘˜ relative to the bias toward the median value that brings about smoothness and kills the noise. We update our estimator as follows:

π‘₯π‘˜(𝑛+1)=argminπ‘§π‘’πœ†(𝑧;π‘₯π‘˜βˆ’1(𝑛),π‘₯π‘˜+1(𝑛),π‘¦π‘˜),π‘˜=0,1,…,𝑁.

(i) Show that when πœ†=1 we have

π‘₯π‘˜(𝑛+1)=median(π‘₯π‘˜βˆ’1(𝑛),π‘₯π‘˜+1(𝑛),π‘¦π‘˜).

(ii) Define the total cost function as (here we denote 𝑧=(𝑧1,…,𝑧𝑁) while before we denote by 𝑧 a scalar)

πΈΜƒπœ†(𝑧;π‘₯(𝑛),𝑦)=βˆ‘π‘˜=1π‘π‘’πœ†(π‘§π‘˜;π‘₯π‘˜βˆ’1(𝑛),π‘₯π‘˜+1(𝑛),π‘¦π‘˜),

and write the iteration process as

π‘₯(𝑛+1)=argminπ‘§πΈΜƒπœ†(𝑧;π‘₯(𝑛),𝑦).

Show that if the above iteration process converges:

then the limit is the critical point of the cost function

πΈπœ†(𝑧;𝑦)=βˆ‘π‘˜=0𝑁|π‘§π‘˜+1βˆ’π‘§π‘˜|+πœ†βˆ‘π‘˜=1𝑁|π‘§π‘˜βˆ’π‘¦π‘˜|.
Stanford Practice, 12 Applied mathematics, jump processes, integro-differential equations, hydrodynamic limit, diffusion limit

Consider a random walk that does the following. A particle starts at a point π‘₯βˆˆβ„ and has a clock attached to it. The clock rings at a random time 𝜏>0, with β„™(𝜏>𝑑)=exp(βˆ’π‘‘). At that time, the particle jumps from the position π‘₯ to a new position 𝑦1βˆˆβ„π‘›, with

β„™(𝑦1∈𝐴)=∫𝐴𝐾(π‘₯βˆ’π‘§)d𝑧,

for any open set π΄βŠ‚β„. Here, 𝐾(π‘₯) is a fixed rapidly decaying smooth non-negative function such that

βˆ«β„πΎ(π‘₯)dπ‘₯=1.

After the jump the clock is reset and the process starts anew: the particle stays at 𝑦1 until the clock rings, when it jumps to the position 𝑦2 such that

β„™(𝑦2∈𝐴)=∫𝐴𝐾(𝑦1βˆ’π‘§)d𝑧,

and so on.

(i) Fix a bounded continuous compactly supported function 𝑓(π‘₯) and define

𝑒(𝑑,π‘₯)=𝔼(𝑓(𝑋(𝑑))).

Here, 𝑋(𝑑) is the location of the random walk that started at time 𝑑=0 at the location π‘₯. Show that 𝑒(𝑑,π‘₯) satisfies the integro-differential equation

πœ•π‘’(𝑑,π‘₯)πœ•π‘‘=βˆ«βˆ’βˆžβˆžπΎ(π‘₯βˆ’π‘¦)𝑒(𝑑,𝑦)dπ‘¦βˆ’π‘’(𝑑,π‘₯),

with the initial condition 𝑒(𝑑=0,π‘₯)=𝑓(π‘₯)β‰₯0.

(ii) Consider a family of solutions π‘’πœ€(𝑑,π‘₯) to this equation with a fixed smooth compactly supported initial condition π‘’πœ€(0,π‘₯)=𝑓(π‘₯) and the kernel πΎπœ€(π‘₯) of the form πΎπœ€(π‘₯)=πœ€βˆ’π‘›πΎ(π‘₯/πœ€), with a fixed non-negative smooth and compactly supported function 𝐾(π‘₯) that satisfies βˆ«β„πΎ(π‘₯)dπ‘₯=1. Show that the functions π‘€πœ€(𝑑,π‘₯)=π‘’πœ€(𝑑/πœ€,π‘₯) converge, as πœ€β†“0, locally uniformly to a limit and that the limit is the solution to

with some constant 𝐷>0 and the initial condition . Identify the diffusivity 𝐷>0 in terms of the kernel 𝐾(π‘₯).

Stanford Practice, 13 Applied mathematics, symmetric hyperbolic systems, energy conservation, first-order PDE systems

Let 𝐴 be a symmetric positive definite π‘šΓ—π‘š matrix, 𝐷𝑗, 𝑗=1,…,𝑛, be symmetric matrices, and let 𝑣=(𝑣1,…,π‘£π‘š) be the vector solution to the system

π΄πœ•π‘£πœ•π‘‘+βˆ‘π‘—=1π‘›π·π‘—πœ•π‘£πœ•π‘₯𝑗=0,𝑑>0,π‘₯βˆˆβ„π‘›,

with the initial condition 𝑣(0,π‘₯)=𝑣0(π‘₯) that is smooth and rapidly decaying at infinity. Show that the energy defined as

is a conserved quantity: 𝐸(𝑑)=𝐸(0) for all 𝑑β‰₯0.

Stanford Practice, 14 Applied mathematics, viscous Burgers' equation, traveling waves, shock profiles, dispersive regularization

Consider the following two regularizations of the Burgers' equation:

𝑒𝑑+𝑒𝑒π‘₯=πœ€π‘’π‘₯π‘₯,

and

𝑣𝑑+𝑣𝑣π‘₯=πœ€π‘£π‘₯π‘₯π‘₯,

where πœ€>0 is a fixed number (you should think of it as being small).

(i) Look for special solutions of the first equation of the form 𝑒(𝑑,π‘₯)=π‘ˆ(π‘₯βˆ’π‘π‘‘) with π‘ˆ(π‘₯) such that π‘ˆ(π‘₯)β†’1 as π‘₯β†’βˆ’βˆž, π‘ˆ(π‘₯)β†’0 as π‘₯β†’+∞, and appropriately chosen 𝑐, and such that 0<π‘ˆ(π‘₯)<1 for all π‘₯βˆˆβ„. (Hint: get an ODE for π‘ˆ(π‘₯) and solve it.) You may assume that all derivatives of π‘ˆ(π‘₯) tend to zero at infinity. This is a viscous approximation of the inviscid shock.

(ii) Show that the second equation has no such solution for 𝑣(𝑑,π‘₯).

Stanford Practice, 15 Applied mathematics, wave equation, finite speed of propagation, energy estimates

Consider the PDE

π‘’π‘‘π‘‘βˆ’βˆ‡β‹…(𝑐2(π‘₯)βˆ‡π‘’)=0,𝑑>0,π‘₯βˆˆβ„π‘›,

with an initial condition 𝑒(0,π‘₯)=𝑓(π‘₯), 𝑒𝑑(0,π‘₯)=𝑔(π‘₯). Here, 𝑓(π‘₯) and 𝑔(π‘₯) are smooth bounded functions, and 𝑐(π‘₯) is a smooth function such that there exist 𝑐1>0, 𝑐2>0 so that 𝑐1≀𝑐(π‘₯)≀𝑐2 for all π‘₯βˆˆβ„π‘›.

(i) Fix π‘₯0βˆˆβ„π‘› and 𝑅0>0 and for 0<𝑑<𝑅0/𝑐2 define

𝐸(𝑑)=∫|π‘₯βˆ’π‘₯0|<𝑅0βˆ’π‘2𝑑(𝑒𝑑2(𝑑,π‘₯)+𝑐2(π‘₯)|βˆ‡π‘’(𝑑,π‘₯)|2)dπ‘₯.

Show that

d𝐸d𝑑≀0for all0<𝑑<𝑅0/𝑐2.

(ii) Suppose that 𝑓(π‘₯)=𝑔(π‘₯)=0 for all π‘₯βˆˆβ„π‘› such that |π‘₯|β‰₯𝑅. Show that 𝑒(𝑑,π‘₯)=0 if |π‘₯|β‰₯𝑅+𝑐2𝑑, so that waves propagate at most with the speed 𝑐2.

Stanford Practice, 16 Applied mathematics, heat equation, Gaussian kernel, decay estimates

Let 𝑒(𝑑,π‘₯) be the solution to the heat equation

πœ•π‘’πœ•π‘‘=𝑒π‘₯π‘₯,𝑑>0,π‘₯βˆˆβ„,

with an initial condition 𝑒0(π‘₯)βˆˆπΆπ‘(ℝ).

(i) Show that there exists a constant 𝑀>0 that depends on 𝑒0 so that

|𝑒π‘₯(𝑑,π‘₯)|≀𝑀𝑑,for allπ‘₯βˆˆβ„and𝑑>0,

and

|π‘₯𝑑𝑒(𝑑,π‘₯)|≀𝑀𝑑,for allπ‘₯βˆˆβ„and𝑑>0.

(ii) Consider the function

𝑀(𝑑,π‘₯)=𝑒π‘₯(𝑑,π‘₯)+π‘₯2𝑑𝑒(𝑑,π‘₯).

Show that 𝑀(𝑑,π‘₯) satisfies

𝑀𝑑=𝑀π‘₯π‘₯βˆ’π‘€π‘‘,

and that there exists 𝐾>0 that depends on 𝑒0 such that

|𝑀(𝑑,π‘₯)|≀𝐾𝑑3/2,for allπ‘₯βˆˆβ„and𝑑>0.

(iii) Use part (i) to estimate how close 𝑒(𝑑,π‘₯) is to the Gaussian

𝐺(𝑑,π‘₯)=14πœ‹π‘‘π‘’βˆ’|π‘₯|2/(4𝑑).
Stanford Practice, 17 Applied mathematics, Legendre transform, convex duality

(i) Let 𝐻(𝑝)=|𝑝|π‘Ÿ/π‘Ÿ, for some π‘Ÿβˆˆ(1,∞). Show that its Legendre transform is 𝐿(𝑦)=|𝑦|𝑠/𝑠 with π‘ βˆˆ(1,∞) satisfying 1/π‘Ÿ+1/𝑠=1.

(ii) Let π‘Žπ‘–π‘— be a symmetric positive-definite matrix, and π‘βˆˆβ„π‘›, and set

𝐻(𝑝)=12βˆ‘π‘–,𝑗=1π‘›π‘Žπ‘–π‘—π‘π‘–π‘π‘—+βˆ‘π‘–=1𝑛𝑏𝑖𝑝𝑖.

Compute its Legendre transform.

Stanford Practice, 18 Applied mathematics, Hopf-Lax formula, Hamilton-Jacobi equations, finite speed of propagation

Suppose that a function β„Ž(π‘₯) satisfies |β„Ž(π‘₯)|≀𝑀(1+|π‘₯|) with some constant 𝑀>0, and 𝐻(𝑝) is a convex function that is super-linear at infinity:

lim|𝑝|β†’+∞𝐻(𝑝)|𝑝|=+∞.

Set

𝑒(π‘₯,𝑑)=minπ‘¦βˆˆβ„π‘›(𝑑𝐿(π‘₯βˆ’π‘¦π‘‘)+β„Ž(𝑦)),

where 𝐿(𝑦) is the Legendre transform of 𝐻(𝑝). Show that actually

𝑒(π‘₯,𝑑)=minπ‘¦βˆˆπ΅(π‘₯,𝑅𝑑)(𝑑𝐿(π‘₯βˆ’π‘¦π‘‘)+β„Ž(𝑦)),

where 𝑅=supπ‘₯βˆˆβ„π‘›|βˆ‡π»(βˆ‡β„Ž(π‘₯))|. Use this to show that Hamilton-Jacobi equations have a finite speed of propagation.

Stanford Practice, 19 Applied mathematics, semilinear elliptic PDE, monotone iteration, Liouville equation

Let Ξ©βŠ‚β„π‘› be a bounded domain with a smooth boundary.

(i) Fix πœ†>0 and consider a sequence of functions defined as follows: 𝑒0≑0 and, given 𝑒𝑛, the function 𝑒𝑛+1 is the solution of the Poisson equation

βˆ’Ξ”π‘’π‘›+1=πœ†π‘’π‘’π‘›(π‘₯),π‘₯∈Ω,

with the boundary condition 𝑒𝑛+1(π‘₯)=0 for π‘₯ on the boundary πœ•Ξ©. Show that 𝑒1(π‘₯)β‰₯𝑒0(π‘₯) for . Use induction to show that 𝑒𝑛+1(π‘₯)β‰₯𝑒𝑛(π‘₯) for all .

(ii) If the limit 𝑒(π‘₯) of 𝑒𝑛(π‘₯) exists then it satisfies

βˆ’Ξ”π‘’=πœ†π‘’π‘’,π‘₯∈Ω,

with the boundary condition 𝑒(π‘₯)=0 for π‘₯ on the boundary πœ•Ξ© (you do not need to prove this). Show that there is so that this equation can not have a non-negative solution for .

Stanford Practice, 2 Applied mathematics, Helmholtz equation, fundamental solutions, decay at infinity

Let 𝑓(π‘₯), π‘₯βˆˆβ„π‘› be a smooth and compactly supported function and π‘˜>0 and consider the following PDE:

βˆ’Ξ”π‘’+π‘˜2𝑒=𝑓(π‘₯),π‘₯βˆˆβ„π‘›.

(i) Show that this equation has a unique bounded solution that decays at infinity.

(ii) Is this true if π‘˜=0? Does the answer depend on dimension?

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