<< Chapter < Page Chapter >> Page >
In this module we provide an overview of the relationship between L1 minimization and random projections of the cross-polytope.

The analysis of 1 minimization based on the restricted isometry property (RIP) described in "Signal recovery in noise" allows us to establish a variety of guarantees under different noise settings, but one drawback is that the analysis of how many measurements are actually required for a matrix to satisfy the RIP is relatively loose. An alternative approach to analyzing 1 minimization algorithms is to examine them from a more geometric perspective. Towards this end, we define the closed 1 ball, also known as the cross-polytope :

C N = x R N : x 1 1 .

Note that C N is the convex hull of 2 N points { p i } i = 1 2 N . Let Φ C N R M denote the convex polytope defined as either the convex hull of { Φ p i } i = 1 2 N or equivalently as

Φ C N = y R M : y = Φ x , x C N .

For any x Σ K = x : x 0 K , we can associate a K -face of C N with the support and sign pattern of x . One can show that the number of K -faces of Φ C N is precisely the number of index sets of size K for which signals supported on them can be recovered by

x ^ = argmin z z 1 subject to z B ( y ) .

with B ( y ) = { z : Φ z = y } . Thus, 1 minimization yields the same solution as 0 minimization for all x Σ K if and only if the number of K -faces of Φ C N is identical to the number of K -faces of C N . Moreover, by counting the number of K -faces of Φ C N , we can quantify exactly what fraction of sparse vectors can be recovered using 1 minimization with Φ as our sensing matrix. See  [link] , [link] , [link] , [link] , [link] for more details and  [link] for an overview of the implications of this body of work. Note also that by replacing the cross-polytope with certain other polytopes (the simplex and the hypercube), one can apply the same technique to obtain results concerning the recovery of more limited signal classes, such as sparse signals with nonnegative or bounded entries  [link] .

Given this result, one can then study random matrix constructions from this perspective to obtain probabilistic bounds on the number of K -faces of Φ C N with Φ is generated at random, such as from a Gaussian distribution. Under the assumption that K = ρ M and M = γ N , one can obtain asymptotic results as N . This analysis leads to the phase transition phenomenon, where for large problem sizes there are sharp thresholds dictating that the fraction of K -faces preserved will tend to either one or zero with high probability, depending on ρ and γ   [link] .

These results provide sharp bounds on the minimum number of measurements required in the noiseless setting. In general, these bounds are significantly stronger than the corresponding measurement bounds obtained within the RIP-based framework given in "Noise-free signal recovery" , which tend to be extremely loose in terms of the constants involved. However, these sharper bounds also require somewhat more intricate analysis and typically more restrictive assumptions on Φ (such as it being Gaussian). Thus, one of the main strengths of the RIP-based analysis presented in "Noise-free signal recovery" and "Signal recovery in noise" is that it gives results for a broad class of matrices that can also be extended to noisy settings.

Questions & Answers

A golfer on a fairway is 70 m away from the green, which sits below the level of the fairway by 20 m. If the golfer hits the ball at an angle of 40° with an initial speed of 20 m/s, how close to the green does she come?
Aislinn Reply
cm
tijani
what is titration
John Reply
what is physics
Siyaka Reply
A mouse of mass 200 g falls 100 m down a vertical mine shaft and lands at the bottom with a speed of 8.0 m/s. During its fall, how much work is done on the mouse by air resistance
Jude Reply
Can you compute that for me. Ty
Jude
what is the dimension formula of energy?
David Reply
what is viscosity?
David
what is inorganic
emma Reply
what is chemistry
Youesf Reply
what is inorganic
emma
Chemistry is a branch of science that deals with the study of matter,it composition,it structure and the changes it undergoes
Adjei
please, I'm a physics student and I need help in physics
Adjanou
chemistry could also be understood like the sexual attraction/repulsion of the male and female elements. the reaction varies depending on the energy differences of each given gender. + masculine -female.
Pedro
A ball is thrown straight up.it passes a 2.0m high window 7.50 m off the ground on it path up and takes 1.30 s to go past the window.what was the ball initial velocity
Krampah Reply
2. A sled plus passenger with total mass 50 kg is pulled 20 m across the snow (0.20) at constant velocity by a force directed 25° above the horizontal. Calculate (a) the work of the applied force, (b) the work of friction, and (c) the total work.
Sahid Reply
you have been hired as an espert witness in a court case involving an automobile accident. the accident involved car A of mass 1500kg which crashed into stationary car B of mass 1100kg. the driver of car A applied his brakes 15 m before he skidded and crashed into car B. after the collision, car A s
Samuel Reply
can someone explain to me, an ignorant high school student, why the trend of the graph doesn't follow the fact that the higher frequency a sound wave is, the more power it is, hence, making me think the phons output would follow this general trend?
Joseph Reply
Nevermind i just realied that the graph is the phons output for a person with normal hearing and not just the phons output of the sound waves power, I should read the entire thing next time
Joseph
Follow up question, does anyone know where I can find a graph that accuretly depicts the actual relative "power" output of sound over its frequency instead of just humans hearing
Joseph
"Generation of electrical energy from sound energy | IEEE Conference Publication | IEEE Xplore" ***ieeexplore.ieee.org/document/7150687?reload=true
Ryan
what's motion
Maurice Reply
what are the types of wave
Maurice
answer
Magreth
progressive wave
Magreth
hello friend how are you
Muhammad Reply
fine, how about you?
Mohammed
hi
Mujahid
A string is 3.00 m long with a mass of 5.00 g. The string is held taut with a tension of 500.00 N applied to the string. A pulse is sent down the string. How long does it take the pulse to travel the 3.00 m of the string?
yasuo Reply
Who can show me the full solution in this problem?
Reofrir Reply
Got questions? Join the online conversation and get instant answers!
Jobilize.com Reply

Get Jobilize Job Search Mobile App in your pocket Now!

Get it on Google Play Download on the App Store Now




Source:  OpenStax, An introduction to compressive sensing. OpenStax CNX. Apr 02, 2011 Download for free at http://legacy.cnx.org/content/col11133/1.5
Google Play and the Google Play logo are trademarks of Google Inc.

Notification Switch

Would you like to follow the 'An introduction to compressive sensing' conversation and receive update notifications?

Ask