## Tuesday, February 06, 2018

## Monday, January 29, 2018

## Thursday, January 25, 2018

## Friday, January 12, 2018

### Tensor squares entangle.

The context involves a pair of particles
which we will assume to be electrons for simplicity.
Let X_{n} measure the spin of the nth electron
with respect to the x-axis.
Applying X_{n} will put the nth electron's spin
in the +x or -x direction;
the corresponding macroscopic observation
will be +1 or -1 (ignoring physical units).
Let Y_{n} be the analog of X_{n} for the y-axis.
If we measure with X_{n} then Y_{n} then X_{n} again,
then the first and second X_{n} measurements
merely have a 1/2 chance of being the same.
In general, if spin of an electron is along one axis
and we measure its spin with respect to another axis,
we effectively destroy information.
(Technically, the information is not destroyed.
But recovering it is like unscrambling an egg.)

The above information loss is algebraically manifested
as X_{n} and Y_{n} not commuting. However,
these operators
do *anti-commute*: X_{n}Y_{n}=-Y_{n}X_{n}.
Therefore, assuming our two electrons' spin states
are independent of each other
(which is approximately true if the electrons are not too close together),
a little algebra shows that the tensor products
X=X_{1}⊗X_{2} and
Y=Y_{1}⊗Y_{2}
do commute.
Physically, this means that if we measure with X then Y then X again,
the two X measurements will agree with probability 1, not 1/2.
If we physically interpret a tensor product
as simply performing two measurements at the same time,
then this makes no sense.

But X actually measures the product of
a potential X_{1} measurement value and
a potential X_{2} measurement value.
This will be +1 if the X_{1} and X_{2} both output +1 or both output -1,
and will be -1 otherwise. In other words, X is measuring merely whether
the two particles have the same or opposite spin with
respect to the x-axis. Unlike an X_{n},
the act of measuring X does not align either particle's
spin to the x-axis (unless it was already there). Instead,
applying X merely changes the joint state of the particles
such that the results of potential future X_{1} and X_{2}
measurements are now either perfectly correlated or
perfectly anti-correlated, depending on whether
X measured +1 or -1.

The bottom line is that, by measuring with X and then Y,
that is, by measuring with respect to each of two perpendicular axes
merely whether our two particles have the same
or opposite spins, we put the two particles into one of four
maximally entangled
joint states with the very nice property that
repeated measurements of X *and* Y
will preserve the joint state of the electrons.
If the X output changes or the Y output ever changes
when performing these repeated measurements,
that indicates outside "noise."
This is a simple instance of quantum error detection for two qubits.
With more electrons, the paper explains
how to achieve quantum error *correction*.

## Monday, January 08, 2018

## Saturday, January 06, 2018

## Thursday, January 04, 2018

## Friday, November 24, 2017

## Tuesday, November 21, 2017

## Tuesday, November 14, 2017

## Saturday, September 09, 2017

## Tuesday, September 05, 2017

## Wednesday, July 12, 2017

[T]here is a significant and fairly large (16% without covariates in the model, 14% with) difference in odds of passing the course for those randomized to the intro stats course compared to the elementary algebra course...Yep. And statistics is more directly useful for non-STEM majors who, for example, want to understand the news.I will hold with Hacker in suggesting that this does represent a lowering of standards, and that this is a feature, not a bug. That is, I think we should allow some students to avoid harder math requirements precisely because the current standards are too high. Students in deeply quantitative fields will have higher in-major math requirements anyway.

I also found it interesting that "support workshops" for remedial college algebra students didn't measurably improve pass rates in this study. I'm not sure what to make of that. I suppose it's consistent with my anecdotal, non-randomized-control-trial experience that more conscientious students are both more likely to pass and more likely to take the time to get help from tutors and/or their professors on a regular basis.

## Saturday, July 08, 2017

## Saturday, July 01, 2017

If the Fed wanted 2018 US NGDP to be more than $20T (for example), it could say, "whenever betting markets generally predict 2018 US NGDP under $20T, we will start to buy and hold assets of our choosing, at a rate of $1B the first day and doubling the rate every day thereafter, until betting markets generally predict 2018 US NGDP over $20T."When there is a large negative expected NGDP, the mismatch between downward-sticky wages and much more plastic hiring/firing/layoffs aggregates into a large short-term misallocation of real resources.

Therefore, the Fed should buy whatever it takes to reverse large downward surprises in expected NGDP.

## Monday, June 26, 2017

I remember when the names iteration.mit.edu and recursion.mit.edu were mine; they pointed to my public IPv4 address 18.238.3.106. I don't claim to have done anything innovative with them, but what I did was very educational. I wrote a minimal http server in C++ and hosted a static website with fractal images I created and a Mandelbrot set Java applet I wrote.

I probably never would have been motivated to learn how to write an http server without such public visibility. Security risks? Yes. (I promptly fixed that one.) Despite this, MIT thrived without a NAT for many years. Even if security risks are greater today, firewalls can be made arbitrarily strict without a NAT.

## Monday, June 19, 2017

### A bit of TeX hacking

I've decided that if I state, say, Theorem 2.2.15 but don't prove it until many pages and lemmas later in Section 5, then, for the reader's sake, I should repeat the theorem verbatim, including the original theorem number, immediately before the proof, as opposed to going straight from the proof of Lemma 5.2.33 to "Proof of Theorem 2.2.15." (Granted, if the delay between statement and proof is just for one "Main Theorem" whose statement is easy to remember, then this is not necessary. My decision is in the context of revising a longer paper with several theorems stated early and proved much later.)

%#1 theoremstyle inpute (plain/definition/remark/...) %#2 type of theorem (Theorem/Lemma/Corollary/...) %#3 label of theorem to be repeated %#4 unique new input for \newtheorem %#5 statement of theorem \def\repeattheoremhelper#1#2#3#4#5{ \theoremstyle{#1} \newtheorem*{#4}{#2 \ref{#3}} \begin{#4} #5 \end{#4} } \def\repeattheorem#1#2{ \repeattheoremhelper{plain}{#1}{#2}{repeat#2}{\csname state#2\endcsname} } %usage example %\theoremstyle{plain} %\newtheorem{thm}{Theorem} %... %\def\statemytheorem{blah blah} %\begin{thm}\label{mytheorem}\statemytheorem\end{thm} %... %\repeattheorem{Theorem}{mytheorem} %\begin{proof} %... %\end{proof}

## Saturday, November 19, 2016

## Thursday, November 03, 2016

## Tuesday, October 18, 2016

## Saturday, October 08, 2016

## Thursday, September 22, 2016

## Tuesday, September 20, 2016

## Friday, September 09, 2016

## Wednesday, September 07, 2016

## Monday, August 29, 2016

## Thursday, August 25, 2016

*v=0.2c*? (See also this.)

Bottom line: I am seriously entertaining the possibility that I will live to see digital images transmitted from another planetary system.