Přepis řeči - ANALYTICAL PERFORMANCE ASSESSMENT OF 1-D STRUCTURED LEAST SQUARES

0:00:13	alright right
0:00:14	welcome everybody thanks for coming to my talk uh i'd as already mentioned that's doesn't order performance analysis for distortion
0:00:19	structure chorus
0:00:20	and it's one of me and and uh for some and her from him and a you know
0:00:24	the call
0:00:25	now for brief more i probably don't have to tell you that high resolution is interesting for a number of
0:00:30	applications
0:00:31	uh in particular is pretty type parameter estimation schemes are often used
0:00:35	because the very simple the very flexible they can be a that the very settings setting closed form you don't
0:00:39	need any peak search or something
0:00:41	and they were perform still close to the cramerrao about
0:00:44	um
0:00:45	and the were based this all this pretty have all "'em" the based on the should than write equation which
0:00:49	are a set of were determined equations which are typically solved using just score
0:00:53	speakers it's a
0:00:55	oh have release is actually suboptimal
0:00:57	it is suboptimal because it you know was more is the fact that there are also estimation errors in the
0:01:02	subspace itself
0:01:03	there is a better technique which is called structure these scores which takes this estimation errors into account and also
0:01:08	explicitly exploits the structure of shift write equations
0:01:11	just been proposed in ninety seven
0:01:14	um so it comes of improve the form
0:01:16	a however the problem is that so far to be scored this is pretty was only evaluated uh a using
0:01:21	the simulations so there is no analytical statement for when does it to for better how much so an analytical
0:01:27	performance evaluation is of course pretty is the a desirable
0:01:30	um the goal here
0:01:32	this paper was to apply to
0:01:33	seem frame we used
0:01:35	if only had to analyse a these scores based pretty
0:01:38	which is this paper by a by car gives the
0:01:40	a a or expansion of of the signal subspace
0:01:44	and i'm in order to analyse a structure discourse basis pretty
0:01:47	we use the same frame of before to analyse these based pretty the corresponding graph
0:01:51	solicit down here
0:01:53	a so we analyzed various versions like standard is pretty unitary esprit read or is pretty in and more you
0:01:57	can even do would for non circular esprit in and others
0:02:00	but no those are based on these scores
0:02:02	oh the purpose you was to extend the no to incorporate structured
0:02:06	uh which brings me to outline of their the the big one iteration we had now i'll go to would
0:02:11	be for usual on you again the shift invariance equations
0:02:13	uh and and what is to actually scores mean showing you the concept of the first-order perturbation for the S
0:02:18	P which you might find interesting to use also in other fields
0:02:21	and and then our earlier phones results for these process pretty in and the main part of focus on structure
0:02:26	these scores of to the solution and then you know as
0:02:28	and in some simulation results
0:02:30	so let's start of the review
0:02:32	a what is what is shift invariance is pretty based on the fact that you can divide the rate into
0:02:36	two identical sub arrays to one and J two which of their of the same observations except for phase shift
0:02:43	but which is encoded in this musical all spatial frequency
0:02:46	and a spatial frequencies link to your parameters of interest for instance if you want to do direction of arrival
0:02:51	name to the direction of arrival and T done a simple relation
0:02:54	now these matrices you you you can use selection make J one and J two which operate on your race
0:02:59	during vector a to select the of the first and the second sub array
0:03:03	and shift them very close to you get the same observation except for a face should which contains the problem
0:03:07	of interest
0:03:08	does is for a single source for multiple source
0:03:11	these J one and J two they operate on the race hearing matrix a which contains all the raised and
0:03:15	vectors
0:03:16	and you parameters is of interest are actually five
0:03:18	right right these contains spatial free
0:03:21	no this is of the right equation a matrix equation the problem is the array steering matrix of course and
0:03:25	no
0:03:26	so to get rid of the unknown array steering matrix
0:03:29	what we do is we take our observations let's say X is the is a is a matrix which contains
0:03:33	and sit C but observations of or and and sensors
0:03:36	and we just computed as P D in from the svd P get an estimate for the signal subspace which
0:03:41	are the D don't the left single vector
0:03:43	and then you was the fact that the race during matrix and this made use S and the same column
0:03:48	space approximately because there is noise
0:03:50	so they are related via a transfer matrix T
0:03:52	and this can be used to eliminate right some we are actually have a shift invariance equations which need to
0:03:57	be sold pop i that's the only known
0:04:00	you has we have an estimate for
0:04:01	and i the eigen base so i are are are do once correct range
0:04:05	right this is the basis for is pretty just a very quick review
0:04:08	the main point here is that these of the shift write equations we need to solve the are determined
0:04:12	and we have an estimate for the subspace but it's not accurate
0:04:15	right
0:04:15	so how do we sell
0:04:17	typically people sold just using these were
0:04:19	and these score just mean to minimize the least squares fit between the left and the right hand side of
0:04:23	the equation right only subject to side
0:04:25	uh this gives a very close from solution a very simple one you can use the inverse
0:04:29	but the problem is you we more the fact that you don't know exactly us that is you actually implicitly
0:04:34	that it's perfectly known which is not true we know that there is in there
0:04:38	and that's the idea of structure these chorus
0:04:40	such each score as change this cost function what is to change here
0:04:43	a change to incorporate for each of these occurrences of the subspace bayes us an additional they'll tell us which
0:04:48	explicitly models the fact that we have an estimation error in the subspace that we tried to correct so that
0:04:54	the two sides of the question a line in a better way
0:04:56	and in an in a group regularization term is to make sure that this up would doing a small to
0:05:01	penalise to lot of
0:05:03	this is the cost function for structure these scores
0:05:05	the nice thing is that takes into account errors and subspace
0:05:08	but draw a always done now not only in your course anymore but it's quadratic
0:05:12	so we typically so it iteratively via a local linearization
0:05:15	but it has been shown that only very few iterations are required actually in the high snr regime only one
0:05:20	iteration is required so you can see just as a as a correct
0:05:24	alright right
0:05:24	now to to to come to the performance analysis for this we need to look into this
0:05:28	source of error that actually here the source of average is here is this yeah to yes this error and
0:05:33	the signal subspace we need to analytically grass
0:05:36	and the the frame up we using for this is the one that by but kind of which i just
0:05:40	briefly you want to review was also very simple
0:05:42	you take a look at you and vector or uh observations X not without any noise where you have you
0:05:47	true signal subspace and a to noise subspace if you break again the S
0:05:50	in the presence of noise you only have an estimate so you can say that your estimate signal subspace is
0:05:55	the true one class and error come down
0:05:57	in this trying to find
0:05:58	and for this
0:05:59	for this error and you can always expand into one part which lies in the model bass and one part
0:06:04	which lies in the signal subspace this just because it leads and this N dimensional space so you can always
0:06:08	break it into but two space
0:06:10	and the interpretation of the first component
0:06:13	it's a a of the signal subspace which is in the noise subspace would really model models how much of
0:06:17	the noise leads into the thing as it's how the subspace itself
0:06:20	a raw whereas the second one is our of the signal subspace inside the signal
0:06:25	this one models how the individual singular vectors inside the signal subspace the particular basis we choose how was the
0:06:30	trip right
0:06:31	so obviously the second one plays no role for esprit because the particular basis because the relevant only the first
0:06:37	one
0:06:38	but extensions exist
0:06:40	we only use the first term because the second one's a relevant if you want you can easily incorporate the
0:06:44	second one as well
0:06:45	has been proposed by a car and a you can see it's a very similar expressions of first order expansion
0:06:50	in the noise and which also perturbation
0:06:52	and the second one it's been proposed actually minor college
0:06:55	um but as i said we don't need for this work
0:06:58	um also the colour already ninety three has used this result to analyse standard esprit in is given a first
0:07:03	order expansion for the estimation error indicates spatial frequency using standard esprit which is the simple expression
0:07:09	based on this work with expanded it
0:07:11	um we've be shown that a last year at i cast in in dallas that you can instance perform statistical
0:07:16	expectation of this
0:07:17	assuming white complex gaussian noise
0:07:19	so what it should probably emphasise that this framework
0:07:22	its asymptotic
0:07:23	in the effective snr so you don't need a large number of snapshots of something
0:07:28	uh you you can have a single snapshot if you want as long as the variance is low and it
0:07:31	needs no a particular assumptions about the statistics you don't need gaussian of the noise you don't even need a
0:07:37	gaussian of the symbols you just need the perturbation to be small
0:07:40	but if you as young gas and then you can of course conforms forms that exceed the expectation and you
0:07:43	get needs better
0:07:45	this is lisa and of this read this is nice unitary we and you can do more
0:07:48	these a previous results we shown and based on these now we try to expand them to incorporate structure
0:07:54	so
0:07:55	um what is done here is we first check our extension attention to a special piece of stuff to these
0:07:59	scores which is using a single iteration
0:08:01	and it is not using any regularization
0:08:03	the reason for this is that these assumptions are asymptotically optimal for structured these in the high snr regime
0:08:09	and since the performance and as we do use anyways asymptotic high as are it's it's fine to assume this
0:08:14	right "'cause" it
0:08:15	but it but it asymptotically in you're actually
0:08:17	right
0:08:18	uh i'm of these assumptions you can express the cost function and the solution and in a very simple way
0:08:22	you can say that these solutions sites for structure these is equal to the initial solution get "'em" by this
0:08:27	first plus an update or
0:08:29	and is a a term is the solution of this cost function
0:08:32	which is of course quadratic "'cause" i've said
0:08:34	there is there is a a a a a term image does not depend on a there is a link
0:08:37	at time and then there is a quadratic term right
0:08:39	the quadratic term be black that's the linearization so we are back to a lean this squares problem
0:08:44	and this mean of this problem has of course of very simple solution
0:08:47	for for us uh to be suppressed so this will be the update for me to in this would be
0:08:51	the update for the for the subspace if if you would wanna do the second iteration be actually don't need
0:08:56	the second
0:08:56	since we only going one
0:08:58	so that the main message here is that it actually the up they can be explicitly computed as taking this
0:09:02	vector are are last
0:09:04	which is the vectorized version of the residual matrix after doing least
0:09:08	a be multiplied by that to them as of this matrix F
0:09:11	which is the linear mapping me
0:09:12	and for this we have to find of a first-order expansion
0:09:15	how have we done it we done it by looking at both terms individually
0:09:19	we start with a
0:09:19	first that's of most of that matrix F
0:09:22	what we will the set you can express this matrix a had as equal to and matrix a matrix they'll
0:09:28	have
0:09:29	but the matrix F is constant in the sense that that does not depend on the perturbation itself self right
0:09:34	so if you look at one realisation look at the random of some of perturbation
0:09:37	this some will be constant and this one will be linear right and this gives the matrix F
0:09:42	and therefore if we look at it so inverse since this part is zero mean it's not very hard to
0:09:46	see a that in versus actually equal to the sort inverse of this constant matrix independent of the perturbation
0:09:51	loss a linear term that's a quadratic term plus i wouldn't for
0:09:54	right we don't actually physically need to spend it it's fine to know that
0:09:58	this constant term as we will see the in terms actually not need and this is simplified and is greatly
0:10:02	and for the second term from those are last
0:10:05	uh it's not difficult to see that this can be written as a a a a at the linux pension
0:10:09	for the again
0:10:10	uh the error in the subspace they are U S be multiplied by one matrix mapping the subspace you to
0:10:15	the residual are possible direct term which be more
0:10:18	and uh also this
0:10:20	a a the subspace is the result of a car
0:10:22	has a mean expansion in terms of the actual perturbation them noise
0:10:25	again but forming that a matrix plus a body matrix plus i don't for
0:10:30	now the collect both
0:10:31	if we collect um this and this together we see that the uh a vector all has a lean expansion
0:10:36	and the noise
0:10:37	and now we combine these two results back into the original expression
0:10:41	we can see that if you multiply the um and this one out them be get a linear term which
0:10:46	is this constant term times the leading it
0:10:48	plus a quadratic term just as linear times the the linear to right so the quadratic term again be like
0:10:54	that's
0:10:54	that's first order
0:10:55	so this shows that we don't actually need even the lean expansion of them soon
0:10:59	right
0:10:59	and then we get this very simple result
0:11:01	a which is pretty into it if you start of the noise you have one a mapping matrix from the
0:11:05	noise to the subspace that from the stuff to the residuals and then this matrix here
0:11:09	this is to the vector and selling and us
0:11:11	but as is that are only interested in this up part
0:11:13	so the final result for this upper part is actually this one again
0:11:17	pretty intuitive meaning about mapping
0:11:19	and uh then you can also like in of back to the original expansion of the estimation error you find
0:11:23	a first or expansion of the estimation error of spatial frequencies again
0:11:27	it's a very simple and it has a form just again in its structure very simple to but these press
0:11:32	expansion be shown previously
0:11:34	are we have a me this vector are L as now it's R S L a slightly different but the
0:11:37	form still the same
0:11:39	and again you can if you want a for means mean
0:11:42	um
0:11:43	the the mean square error if you assume as your mean and circle is much white noise you actually don't
0:11:47	you gals in for this
0:11:48	and you get a needs got are again very compact and and simplex spray
0:11:51	now but is all this good for why do we do a why do we go through this analytical result
0:11:55	and what does it show us now that we have the result
0:11:57	the break
0:11:58	think this is good for is if you look at
0:12:00	that's
0:12:00	specific case we can simplify the expression so much that you actually gain inside
0:12:05	in to what is the performance of the schemes of the very specific set
0:12:09	and to to add the this point i brought one example you which is not the paper due to like
0:12:13	of space but i still i think it's interesting
0:12:15	to kind of push for what of it that this we has has applications
0:12:18	and the example is of course the simple one you can think of which is a single source
0:12:22	if you consider a single sauce
0:12:24	and be shown the uh that fully score space is pretty the means error as a break
0:12:28	compact expression if you consider a uniformly a rate of N sensors
0:12:32	um it has to be effective as an front and then it's quadratic and one over one over and basically
0:12:37	then the common or bound also as a very simple expression
0:12:40	which means that you can find the asymptotic efficiency again asymptotic effective snr it still it's about for single snapshot
0:12:46	um is is given by this expression so you have a closed form expression for the asymptotic efficiency only depending
0:12:51	on and
0:12:52	in it's exact except for the fact that it doesn't talk
0:12:55	um so and and what you can see you is that it basically it's start of one for two and
0:12:59	three sensors and then it goes down
0:13:01	so these press based pretty is not efficient for large race on a single song
0:13:05	we did the same number of the structure these scores
0:13:07	and after a number of manipulations we found again a closed-form expression for the mean square
0:13:12	it's a bit more involved but you can do the same thing you can not of like from are bound
0:13:15	i mean square error and you find a close form expression for the asymptotic efficiency which is
0:13:20	a ratio of order only us
0:13:22	interestingly the first three coefficients agree then they start to diff
0:13:25	if you plot is on the same thing as a things you and one it looks like it's almost equal
0:13:29	to one but is actually not if you zoom in a little bit you can see it starts of one
0:13:33	it goes down a little bit and then it goes back out
0:13:35	we don't really have physical explanation for that mathematically you could prove that it is that with simulations you can
0:13:40	verify that like
0:13:42	and you really you have the values for the asymptotic efficiency as as exact number so this is a pretty
0:13:46	value result
0:13:47	it would be interesting to extend this to two sources to see was the performance in terms of separation correlation
0:13:52	and these real or
0:13:53	uh a parameter stuff
0:13:55	alright right
0:13:55	a just a few must simulations and the simulations will be compared is is we compare the empirical error
0:14:00	which you get by actually performing as free on random data and then computing the estimate the spatial frequencies computing
0:14:06	the arrow an averaging it
0:14:08	with the semi analytical results which still depend on the noise realisations of the average these or noise
0:14:13	and a fully analytical results which which for which no simulations actually needed on the one to colour everything is
0:14:19	needed because there are around of that
0:14:20	right
0:14:21	uh a this first example he for uncorrelated sources
0:14:24	you know the the performance of unitary briefly specified
0:14:28	sort
0:14:28	these grass actually scores
0:14:30	is very close so it's of course interesting to see can this really small gap still be reliably predicted
0:14:35	well the S is yes
0:14:37	with our analytical results we become asymptotically optimal yeah the same small yeah
0:14:41	the semi analytical this
0:14:42	the volume
0:14:43	uh another the result this is pretty source which are very strongly correlated there zero point ninety nine core between
0:14:48	any pair of soft
0:14:49	i know we have four as we have to us and standard this spree based on these press actually scores
0:14:54	unitary esprit based on these cost of is discourse
0:14:56	to do this time correlation or is a big gas so you can more clearly distinguished the curve
0:15:01	again this is the i mean uh the results to become
0:15:03	accurate for high snr this
0:15:05	this
0:15:05	the form you
0:15:06	and then use the single source now for single source we have an improvement if you plot of versus the
0:15:10	snr
0:15:11	for for eight sensors between these grass structure course
0:15:14	and again the analytical results
0:15:17	but range to the conclusions
0:15:18	what we present a is a first order
0:15:20	a a perturbation analysis to actually score is pretty
0:15:23	just based on the performance analysis for the S D which is a very nice concept that can be used
0:15:27	also in different field
0:15:29	the nice thing about it its asymptotic and the effective snr so i a small noise variance
0:15:33	well a large and
0:15:34	can be both for whatever you want
0:15:36	and it explicit which means you don't need any assumptions about the statistics you need to noise to be zero
0:15:41	mean but you don't need to source to be gaussian you the noise to be C
0:15:44	you just need to be small
0:15:46	and is also shown means but our assuming zero-mean circular is met guide noise
0:15:50	and now also shown the explicit expressions for single source where you can actually see just talking
0:15:55	this concludes my talk things
0:16:03	we have time for question
0:16:14	yeah
0:16:15	there is a relation but there is also a difference
0:16:18	um
0:16:19	okay here
0:16:20	in an in totally scores you allow for an error
0:16:23	in in in this expression in you mean mapping matrices that's say
0:16:27	but you assume that there as are independent errors on the left and the right hand side of spray
0:16:32	at that's why this is called structure these course totally suppressed would model to independent errors for the left and
0:16:37	the right and say the different
0:16:38	i actually there is a structure in the shift writes equations which tells you that these are actually not and
0:16:42	pain and are almost the same except little selection matrices
0:16:45	and the structure should be incorporated the solution
0:16:51	yeah
0:16:52	yeah
0:16:54	right
0:16:55	this only is yeah
0:16:56	yeah
0:17:16	it doesn't have to be we don't can find that that that you explicitly to be unit
0:17:20	it could be not
0:17:25	well
0:17:25	you for for is pretty you don't need a constraint that does unitary mean
0:17:29	this you can you to any subspace at you one doesn't have to be you know
0:17:39	but you can you can describe a sub using any is any base equivalent typically you the S D because
0:17:44	it gives you know from all the basis and it's nice to work with and it's simple
0:17:48	but you could use any other basis and it would have no inter
0:17:51	form
0:17:51	any base
0:17:52	fine
0:17:53	actually me started rolling taxes pretty the first version
0:17:56	i'll be defined of subspace it was long units are you but then when be corrected it we met every
0:18:00	had no impact on the performance which is
0:18:02	just would be
0:18:03	yeah but just
0:18:06	us us this to be unitary domain
0:18:10	if you had last yeah i
0:18:12	not so mean unit
0:18:13	mean
0:18:14	so can you
0:18:15	the
0:18:16	i you know a
0:18:17	to to issue
0:18:18	you would like to minimize
0:18:20	but which
0:18:21	know
0:18:22	you would still operate
0:18:23	you can men
0:18:24	C
0:18:25	yeah
0:18:27	you could do would but i one
0:18:28	you you what what would be the uh the data
0:18:30	i mean we don't need to same unitary T four
0:18:34	the writing is pretty for using it
0:18:37	but it would be possible
0:18:40	i you you have question
0:18:43	a some thought of a set of goes to infinity so a set of the not so sure
0:18:50	i
0:18:50	i
0:18:51	so what we actually need
0:18:52	let me go to
0:18:55	well
0:18:57	what we need is that this term and frame here that it they can zero we and P D which
0:19:01	is the power of sauce of single and which is the power of your
0:19:04	um and the the noise variance and you and which is the number of snapshots
0:19:08	so if you have a finite snr and you that in going to infinity works just exactly the same way
0:19:13	i i you let and go to infinity or you get the noise variance go zero all
0:19:17	a source power go to
0:19:18	in
0:19:27	yes it single source only for singles
0:19:30	it's not as bad for for multiple
0:19:34	it was a prize one as what for the first time but i can very fight using selection
0:19:37	so
0:19:41	it is surprising because he the low resolution techniques are asymptotically optimal for single source but it's is not
0:19:53	when when that more sources is it it's not as that it's it's very hard to find as expressions explicitly
0:19:57	for most source because the number of terms get
0:19:59	it's very large
0:20:00	very to use we try simplify simplified
0:20:02	we we we actually didn't
0:20:03	get the final result but from from simulations my experience is that
0:20:06	this kind of the the risk case in terms of comparing it with rubber
0:20:12	it also disappear of course if you replace quest squares fast a score
0:20:15	which may serve of the spec
0:20:18	and you just it's just one correction term it's not and it to iterative procedure to apply already of a
0:20:23	single iteration it basically disappear
0:20:26	in it's it's something simple it's holding one set of
0:20:29	when
0:20:34	a
0:20:34	oh yeah
0:20:35	the question
0:20:36	it seems that uh stuff to the squares
0:20:39	but and and these squares
0:20:40	especially when the source is a card
0:20:43	right
0:20:44	so okay translate translated
0:20:46	a
0:20:47	so
0:20:48	estimation use
0:20:49	uh
0:20:50	is words
0:20:51	when the sources are quite
0:20:53	is better one one
0:20:55	because this is main
0:20:57	to my
0:20:58	a problem is that
0:21:00	there is not always a one-to-one mapping between
0:21:02	a better self space and a better performance of this pretty
0:21:05	but but start of a senses as for single source we got a better subspace but the the the the
0:21:09	means but our of the speech that's both exact
0:21:12	sometimes times you get you get a better subspace but it does not help Q in terms of your you
0:21:16	mean square
0:21:17	i would say that there should probably be be something but i don't know if it's the weak link
0:21:21	a strong so this something
0:21:22	still have
0:21:26	which
0:21:27	so let's

ANALYTICAL PERFORMANCE ASSESSMENT OF 1-D STRUCTURED LEAST SQUARES

Detection and Estimation

Přednášející: Florian Roemer, Autoři: Florian Roemer, Martin Haardt, Ilmenau University of Technology, Germany