$$
\newcommand{\bs}{\boldsymbol}
\newcommand{\cl}{\mathcal}
\newcommand{\bb}{\mathbb}
$$
This simple *python notebook* aims at estimating the validity of some of the results explained in the paper

"

A Quantized Johnson Lindenstrauss Lemma: The Finding of Buffon's Needle"

by Laurent Jacques (arXiv)

"In 1733, Georges-Louis Leclerc, Comte de Buffon in France, set the ground of geometric probability theory by defining an enlightening problem: What is the probability that a needle thrown randomly on a ground made of equispaced parallel strips lies on two of them? In this work, we show that the solution to this problem, and its generalization to N dimensions, allows us to discover a quantized form of the Johnson-Lindenstrauss (JL) Lemma, i.e., one that combines a linear dimensionality reduction procedure with a uniform quantization of precision $\delta>0$. In particular, given a finite set $\cl S \in \bb R^N$ of $S$ points and a distortion level $\epsilon>0$, as soon as $M > M_0 = O(\log |S|/\epsilon^2)$, we can (randomly) construct a mapping from $(\cl S, \ell_2)$ to $((\delta \bb Z)^M, \ell_1)$ that approximately preserves the pairwise distances between the points of $\cl S$. Interestingly, compared to the common JL Lemma, the mapping is quasi-isometric and we observe both an additive and a multiplicative distortions on the embedded distances. These two distortions, however, decay as $O(\sqrt{\log |S|/M})$ when $M$ increases. Moreover, for coarse quantization, i.e., for high $\delta$ compared to the set radius, the distortion is mainly additive, while for small $\delta$ we tend to a Lipschitz isometric embedding. Finally, we show that there exists "almost" a quasi-isometric embedding of $(\cl S, \ell_2)$ in $((\delta \bb Z)^M, \ell_2)$. This one involves a non-linear distortion of the $\ell_2$-distance in $\cl S$ that vanishes for distant points in this set. Noticeably, the additive distortion in this case decays slower as $O((\log S/M)^{1/4})$."

In particular, our objective is to study the behavior of a nonlinear mapping from $\bb R^N$ to $\bb R^M$, for two specific dimensions $M,N \in \bb N$. This mapping is defined as follows.

Let a random (sensing) matrix $\bs \Phi \in \bb R^{M \times N}$ be such that each component $\Phi_{ij} \sim_{\rm iid} \cl N(0,1)$, or more shorthly $\bs \Phi \sim \cl N^{M\times N}(0,1)$.

We want to combine the common random projection realized by $\bs \Phi$ with the following non-linear operation, i.e., a uniform scalar quantizer of resolution $\delta > 0$:

$$
\qquad\cl Q_\delta[\lambda] = \delta \lfloor \lambda / \delta \rfloor.
$$

(remark: we could define instead a *midrise* quantizer by adding $\delta/2$ to the definition above, and the rest of the development would be unchanged)

This combination reads

$$
\qquad\bs \psi_\delta(\bs x) := \cl Q_\delta(\bs\Phi \bs x + \bs \xi)
$$

with $\bs \xi \sim \cl U^M([0, \delta])$ is a *dithering* vector, i.e., a random uniform vector in $\bb R^M$ such that $u_i \sim_{\rm iid} \cl U([0, \delta])$, and $\bs \psi_\delta:\bb R^N \to (\delta \bb Z)^M$ $ is our mapping of interest.

In Proposition 13 (page 16) of the paper above, it shown that

Proposition 13:Fix $\epsilon_0>0$, $0< \epsilon\leq \epsilon_0$ and $\delta>0$. There exist two values $c,c'>0$ only depending on $\epsilon_0$ such that, for $\bs\Phi \sim \cl N^{M\times N}(0,1)$ and $\bs \xi\sim \cl U^M([0, \delta])$, both determining the mapping $\bs\psi_\delta$ above, and for $\bs u, \bs v\in\bb R^N$,

$$\qquad(1 - c\epsilon) \|\bs u - \bs v\| - c'\epsilon\delta\ \leq\ \tfrac {\sqrt\pi}{\sqrt 2 M} \|\bs\psi_\delta(\bs u) - \bs\psi_\delta(\bs v)\|_1\ \leq\ (1 + c\epsilon)\|\bs u - \bs v\| + c'\epsilon\delta.\tag{1} $$

with a probability higher than $1 - 2 e^{-\epsilon^2M}$.

This proposition shows that the random quantity $c_\psi M^{-1} \|\bs\psi_\delta(\bs u) - \bs\psi_\delta(\bs v)\|_1$ with $c_\psi = \sqrt{\pi/2}$ *concentrates* around its mean $\|\bs u - \bs v\|$. However, conversely to linear random projections, this concentration phenomenon displays two kind of deviation: a standard multiplicative one (the $1\pm c\epsilon$ factor) and an *additive* one in $\pm c'\epsilon\delta$.

Moreover, forcing (1) to be valid at constant probability, we deduce also that $\epsilon = O(1/\sqrt M)$, i.e., showing that both the multiplicative and the additive distortion decay as $O(1/\sqrt M)$ with respect to $M$.

Remark:From a standard union bound argument (see the paper), this result allows one to show the existence of a non-linear embedding from a set $\cl S \subset \bb R^N$ to $(\delta \bb Z)^M$, as soon as $M \geq M_0 = O( \epsilon^{-2}\,\log |\cl S|)$. Proposition 13 is thus central to reach this property.

This notebook proposes to test the behavior of the two distortions displayed in (1).

For that, arbitrarily fixing $\|\bs u - \bs v\|=1$ by normalizing conveniently $\bs u$ and $\bs v$ (e.g., after their random selection in $\bb R^N$), we study the standard deviation of the random variable

$$
\qquad V_\psi = \tfrac{\sqrt\pi}{\sqrt 2 M} \|\bs\psi_\delta(\bs u) - \bs\psi_\delta(\bs v)\|_1.
$$

Remark:the concentration (1) is invariant under the coordinate change $\bs u \to \lambda \bs u$, $\bs v \to \lambda \bs v$ and $\delta \to |\lambda| \delta$ for any $\lambda \neq 0$, which allows us to set $\|\bs u - \bs v\|=1$ without any loss of generality (providing we study the variability of (1) in $\delta$).

Although this random variable displays a non-trivial distribution^{1}, we expect anyway that, if Prop. 13 above is true,

$$
\qquad (\text{Var}\ V_\psi)^{1/2}\quad \simeq\quad a\ \epsilon\ +\ b\epsilon\ \delta,\quad \text{for some }a,b > 0,
$$

and possibly find the constants $a, b>0$ by a simple linear fit.

^{1}: Actually, a mixture of *Buffon* random variable and of a Chi distribution with $N$ degrees of freedom.

Remark:launch ipython notebook with the pylab option, i.e.,

ipython notebook --pylab=inline

In [1]:

```
import numpy as np
```

Defining the $\bs \psi_\delta:\bb R^N \to (\delta \bb Z)^M$ with two functions:

In [2]:

```
def quant(val, d): # the uniform quantizer of resolution 'd'
return d * np.floor(val/d)
```

In [3]:

```
def psi(vec, mat, dith, d): # the mapping (matrix A, dithering u, quantization d)
return quant(mat.dot(vec) + dith, d)
```

*Experimental setup:* The standard deviation of $V_\psi$ is evaluated for several number of measurements $M$ and for several values of $\delta$. For each of them a certain number of trials are generated. We found that for small $M$ a higher number of trials leads to more stable estimation and we set arbitrarily this number to $1024*64/M$ (setting this number to 100 also works but less accurately). As for estimating the restricted isometry property in Compressed Sensing, the sensing matrix $\bs \Phi$, and the dithering $\bs \xi$ as well, are regenerated at every trial.

In [4]:

```
# space dimension
N = 512
c_psi = np.sqrt(np.pi/2) # used for normalizing psi
# variable number of dimensions
M_v = np.array([64, 128, 256, 512, 1024])
nb_M = M_v.size
nb_delta = 8
# The fixed value for ||u - v|| = 1
dist_l2 = 1
# Testing several delta, a logspace arrangement seems logical, here from 10^-3 to 10
delta_v = np.logspace(-3,1,nb_delta)
V_psi_std = np.zeros([nb_M,nb_delta])
# Only the standard deviation of V_psi matters here,
# but interested readers could evaluate its mean too to see that it matches ||u - v||.
# In this case, just uncomment this line and the one
# V_psi_avg = np.zeros([nb_M,nb_delta])
for j in range(nb_M):
M = M_v[j]
# nb_trials = 100 # uncomment for a constant number of trials
nb_trials = 1024*64/M # better stability to have more trials for small M
V_psi = np.zeros(nb_trials) # temporary store distances in the embedded space
for k in range(nb_delta):
for i in range(nb_trials):
# local variables for the loop
delta = delta_v[k]
# Defining the sensing matrix and dithering
Phi = np.random.randn(M,N)
# and dithering, i.e., uniform random vector in [0, \delta]
xi = np.random.rand(M,1)*delta
# Generating two points in R^N and normalizing their distance to 1
tmp_u = np.random.randn(N,1)
tmp_v = np.random.randn(N,1)
tmp_dist_uv = np.linalg.norm(tmp_u - tmp_v)
u = tmp_u * dist_l2 / tmp_dist_uv;
v = tmp_v * dist_l2 / tmp_dist_uv;
# projecting the two points according to psi
u_proj = psi(u, Phi, xi, delta);
v_proj = psi(v, Phi, xi, delta);
# storing one sample of the normalized l1 distance
V_psi[i] = c_psi*np.linalg.norm(u_proj - v_proj,1)/M
V_psi_std[j,k] = np.std(V_psi)
# For mean evaluation, you could estimate too:
# V_psi_avg[j,k] = np.mean(V_psi)
print j, # observing the loop progression (sober progress bar ;-)
```

Let's observe now the diferent evolutions of $V_{\psi}$ vs. $\delta$ for the different number of measurements $M\in \{64, \cdots, 1024\}$ selected above:

In [5]:

```
fig, ax = plt.subplots()
for k in range(M_v.size):
ax.plot(delta_v, V_psi_std[k], '.-', label = "M = %i" % M_v[k])
ax.set_title(r'$({\rm Var}\ V_\psi)^{1/2}$ vs $\delta$')
ax.set_xlabel(r'$\delta$')
ax.set_ylabel(r'$({\rm Var}\ V_\psi)^{1/2}$')
ax.legend(bbox_to_anchor=(1.40, 1))
fig, ax = plt.subplots()
for k in range(M_v.size):
ax.plot(delta_v[0:-1], V_psi_std[k][0:-1], '.-', label = "M = %i" % M_v[k])
ax.set_title(r'$({\rm Var}\ V_\psi)^{1/2}$ vs $\delta$ (zoom on x-axis)')
ax.set_xlabel(r'$\delta$')
ax.set_ylabel(r'$({\rm Var}\ V_\psi)^{1/2}$')
ax.legend(bbox_to_anchor=(1.40, 1))
```

Out[5]:

From this last plot, we conclude that:

- for $\delta \gtrsim 0.2$, $({\rm Var}\ V_\psi)^{1/2}$ displays a linear progression in $\delta$;
- for very small $\delta$ compared to $\|\bs u - \bs v\|=1$, $({\rm Var}\ V_\psi)^{1/2}$ saturates (note that this is
**not**explained by the theory); - for different value of $M$, the linear trend of $({\rm Var}\ V_\psi)^{1/2}$ has an offset as $\delta \simeq 0$;
- the slope and the offset of the linear progresison clearly depend on $M$.

Let's go one step further in our analysis.

From this plot, we perform a linear fit to estimate $(\text{Var}\ V_\psi)^{1/2}$ as

$$
\qquad(\text{Var}\ V_\psi)^{1/2}\quad \simeq\quad v_\alpha +\ v_\beta\ \delta,\qquad \text{for some }v_\alpha, v_\beta > 0,
$$

Actually, we have to estimate one couple of $(v_\alpha,v_\beta)$ for each value $M$, since, from what we explained above, we should have

$$\qquad v_\alpha\ =\ a\ \epsilon$$

and

$$\qquad v_\beta\ =\ b\ \epsilon$$

for some constants $a$ and $b$ and $\epsilon = O(1/\sqrt{M})$ depending on $M$ (at fixed probability for inequality (1) above).

Let us see if this is what we get. We first do the linear fit:

In [6]:

```
# initialization
v_alpha = np.zeros(M_v.size)
v_beta = np.zeros(M_v.size)
# For each M, use np.polyfit at degree 1
for k in range(M_v.size):
v_beta[k], v_alpha[k] = np.polyfit(delta_v, V_psi_std[k], 1)
```

If $v_\beta = b \epsilon$, where we recall that $v_\beta$ is the *slope* of each curves in the plots above, we should see a good match between $v_\beta(M)$ and

$$
\qquad v^{\rm th}_\beta(M)\ :=\ \sqrt{\tfrac{M_0}{M}}\ v_\beta(M_0),\qquad \text{with $v^{\rm th}_\beta(M_0)=v_\beta(M_0)$}
$$

for one fixed value $M_0$.

Is it what we have?

In [7]:

```
plt.semilogx(M_v, v_beta, 'o-', label=r'$v_\beta(M)$')
plt.semilogx(M_v, v_beta[0]*np.sqrt(M_v[0])/np.sqrt(M_v), 'o-', label=r'$v^{\rm th}_\beta(M)$') # M_0 is the first M of M_v
plt.xlabel(r'$M$')
plt.ylabel(r'$\beta$')
plt.axis('tight')
plt.ylim(0, v_beta[0])
plt.legend();
```

The match sounds good enough!

Finally, if we really have $v_\alpha = a \epsilon$ and $v_\beta = b \epsilon$, $v_\beta$ should be a linear function of $v_\alpha$, i.e., $v_\alpha/v_\beta \simeq a/b$.

Let's test this fact.

In [8]:

```
fig, ax = plt.subplots()
ax.plot(v_alpha, v_beta, '.-', label = r'$v_\beta$ vs. $v_\alpha$')
ax.plot(np.linspace(0,v_alpha.max(),10), np.linspace(0,v_alpha.max(),10)*v_beta.max()/v_alpha.max(), label = 'linear trend')
ax.set_xlim(0, v_alpha.max())
ax.set_ylim(0, v_beta.max())
ax.set_xlabel(r'$v_\alpha$')
ax.set_ylabel(r'$v_\beta$')
ax.legend(bbox_to_anchor=(.5, 1))
ratio, offset = np.polyfit(v_alpha,v_beta,1)
print "We approximatley have v_beta = %f v_alpha + %f" % (ratio, offset)
```

Laurent Jacques, November 2013