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In this module we introduce the restricted isometry property (RIP) and discuss its role in compressive sensing. In particular, we describe the relationship between the RIP and the concept of stability in the context of sparse signal acquisition. We also provide a simple lower bound on the number of measurements necessary for a matrix to satisfy the RIP.

The null space property (NSP) is both necessary and sufficient for establishing guarantees of the form

Δ ( Φ x ) - x 2 C σ K ( x ) 1 K ,

but these guarantees do not account for noise . When the measurements are contaminated with noise or have been corrupted by some error such as quantization, it will be useful to consider somewhat stronger conditions. In  [link] , Candès and Tao introduced the following isometry condition on matrices Φ and established its important role in compressive sensing (CS).

A matrix Φ satisfies the restricted isometry property (RIP) of order K if there exists a δ K ( 0 , 1 ) such that

( 1 - δ K ) x 2 2 Φ x 2 2 ( 1 + δ K ) x 2 2 ,

holds for all x Σ K = x : x 0 K .

If a matrix Φ satisfies the RIP of order 2 K , then we can interpret [link] as saying that Φ approximately preserves the distance between any pair of K -sparse vectors. This will clearly have fundamental implications concerning robustness to noise.

It is important to note that in our definition of the RIP we assume bounds that are symmetric about 1, but this is merely for notational convenience. In practice, one could instead consider arbitrary bounds

α x 2 2 Φ x 2 2 β x 2 2

where 0 < α β < . Given any such bounds, one can always scale Φ so that it satisfies the symmetric bound about 1 in [link] . Specifically, multiplying Φ by 2 / ( β + α ) will result in an Φ ˜ that satisfies [link] with constant δ K = ( β - α ) / ( β + α ) . We will not explicitly show this, but one can check that all of the theorems in this course based on the assumption that Φ satisfies the RIP actually hold as long as there exists some scaling of Φ that satisfies the RIP. Thus, since we can always scale Φ to satisfy [link] , we lose nothing by restricting our attention to this simpler bound.

Note also that if Φ satisfies the RIP of order K with constant δ K , then for any K ' < K we automatically have that Φ satisfies the RIP of order K ' with constant δ K ' δ K . Moreover, in  [link] it is shown that if Φ satisfies the RIP of order K with a sufficiently small constant, then it will also automatically satisfy the RIP of order γ K for certain γ , albeit with a somewhat worse constant.

(corollary 3.4 of [link] )

Suppose that Φ satisfies the RIP of order K with constant δ K . Let γ be a positive integer. Then Φ satisfies the RIP of order K ' = γ K 2 with constant δ K ' < γ · δ K , where · denotes the floor operator.

This lemma is trivial for γ = 1 , 2 , but for γ 3 (and K 4 ) this allows us to extend from RIP of order K to higher orders. Note however, that δ K must be sufficiently small in order for the resulting bound to be useful.

The rip and stability

We will see later in this course that if a matrix Φ satisfies the RIP, then this is sufficient for a variety of algorithms to be able to successfully recover a sparse signal from noisy measurements. First, however, we will take a closer look at whether the RIP is actually necessary. It should be clear that the lower bound in the RIP is a necessary condition if we wish to be able to recover all sparse signals x from the measurements Φ x for the same reasons that the NSP is necessary. We can say even more about the necessity of the RIP by considering the following notion of stability.

Questions & Answers

what does the ideal gas law states
Joy Reply
Three charges q_{1}=+3\mu C, q_{2}=+6\mu C and q_{3}=+8\mu C are located at (2,0)m (0,0)m and (0,3) coordinates respectively. Find the magnitude and direction acted upon q_{2} by the two other charges.Draw the correct graphical illustration of the problem above showing the direction of all forces.
Kate Reply
To solve this problem, we need to first find the net force acting on charge q_{2}. The magnitude of the force exerted by q_{1} on q_{2} is given by F=\frac{kq_{1}q_{2}}{r^{2}} where k is the Coulomb constant, q_{1} and q_{2} are the charges of the particles, and r is the distance between them.
Muhammed
What is the direction and net electric force on q_{1}= 5µC located at (0,4)r due to charges q_{2}=7mu located at (0,0)m and q_{3}=3\mu C located at (4,0)m?
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Capacitor is a separation of opposite charges using an insulator of very small dimension between them. Capacitor is used for allowing an AC (alternating current) to pass while a DC (direct current) is blocked.
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A motor travelling at 72km/m on sighting a stop sign applying the breaks such that under constant deaccelerate in the meters of 50 metres what is the magnitude of the accelerate
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Sharon
8m/s²
Aishat
What is Thermodynamics
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velocity can be 72 km/h in question. 72 km/h=20 m/s, v^2=2.a.x , 20^2=2.a.50, a=4 m/s^2.
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A boat travels due east at a speed of 40meter per seconds across a river flowing due south at 30meter per seconds. what is the resultant speed of the boat
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50 m/s due south east
Someone
which has a higher temperature, 1cup of boiling water or 1teapot of boiling water which can transfer more heat 1cup of boiling water or 1 teapot of boiling water explain your . answer
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I believe temperature being an intensive property does not change for any amount of boiling water whereas heat being an extensive property changes with amount/size of the system.
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Scratch that
Someone
temperature for any amount of water to boil at ntp is 100⁰C (it is a state function and and intensive property) and it depends both will give same amount of heat because the surface available for heat transfer is greater in case of the kettle as well as the heat stored in it but if you talk.....
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field is a region of space under the influence of some physical properties
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Two bodies attract each other electrically. Do they both have to be charged? Answer the same question if the bodies repel one another.
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Are you really asking if two bodies have to be charged to be influenced by Coulombs Law?
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like charges repel while unlike charges atttact
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Source:  OpenStax, An introduction to compressive sensing. OpenStax CNX. Apr 02, 2011 Download for free at http://legacy.cnx.org/content/col11133/1.5
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