---------- Forwarded message ----------
From:
Steven White <srwhite@uci.edu>Date: Tue, Mar 30, 2010 at 2:29 AM
Subject: Re: Paper
To: Alan Aspuru-Guzik <
alan@aspuru.com>
Dear Alan,
The mapping looks similar to things I've seen in solid state. I have thought the near-neighbor
coupling could be generated with a fair amount of generality by a Lanczos type procedure--so
I'm not sure how this polynomial version is different.
Regarding the t-DMRG, the paper is missing a section on the calculational details, and references.
This might be like saying "using DFT, we solved this problem and here are the energies" without
ever mentioning which DFT, which basis, etc etc. It is all probably fine, but here are some questions
needing answers in any reasonable paper:
Which version of t-DMRG (reference), which breakup (2nd order Trotter? 4-th order Trotter?) What
time step? How big a lattice? How many time steps? How many states kept? Was the truncation
controlled by a truncation error cutoff or a maximum number of states? What was the accumulated
truncation error? What was the maximum in the number of states kept if the a truncation error cutoff was used?
Can they show any plots with different cutoff criterion for comparison? What do they mean by
numerically exact? (This phrase is sometimes used for regular DMRG in a 1D system, but I've
never heard it used for time dependent DMRG.) How long did the calculations take?
Without these sorts of details one can't really evaluate the t-DMRG part.
Best regards,
Steve
On Tue, Mar 30, 2010 at 1:15 AM, Alan Aspuru-Guzik
<alan@aspuru.com> wrote:
Dear Steven
This is the paper I was talking to you about. Let me know your thoughts on the time evolution aspect.
Best and thanks!
Alan