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next step: positive Lambda
It seems likely that the next step in developing Covariant Loop Gravity will be a continuation of Livine's thesis that introduces positive Lambda----positive dark energy, or cosmological constant---into the theory.
The key new idea we need to grasp is that the "quantum hyperboloid becomes a stack of fuzzy spheres"
see first paragraph page 2 of Girelli/Livine "Quantizing Speeds with the Cosmological Constant" gr-qc/0311032
see also their equation (1)
The basis for "Quantizing Speeds..." is what now seems to be a very important paper by Karim Noui and Philippe Roche "Cosmological Deformation of Lorentzian Spin Foam Models" gr-qc/0211109
and in particular page 13 where the hyperboloid of possible speeds is put in terms of some 2x2 matrices---a right coset homog. space SU(2)\SL(2,C) and the Iwasawa decomposition is used to get it as A x N (diagonal and nilpotent) How bad can it be? It is just a few 2x2 matrices of especially simple form
lambda 0
0 lambda-1
plus
0 0
n 0
the first is the real number diagonal det=1 type
and the second is the complex number n for nilpotent
lower triangular type, the language here is heavier than the matrices
let's see if I can type the sum of those two matrices
so the hyperboloid of possible speeds, or moving observers, or boosts or whatever, is happily pictured algebraically as some 2x2 matrices
NOW Noui/Roche will tell us how to q-deform them by introducing a cosmological constant.
See page 16 and 17
You will see elegant french style. first the quantum hyperboloid is presented in a fearsomely succinct and categorical way, then in equation (55) one sees that it is simply a stack of spheres made of essemtially the same matrices except the lower left entry, the complex number n, has been multiplied by something EXTREMELY NEAR ONE.
and then presto on the next page there is equation (58) that Girelli and Livine used to see the spectrum of quantized speeds.
The fearsome and succinct definition they give first is something else. They refer to the algebra of compactly supported functions on the quantum hyperboloid as
Func(H+q) = Func(ANq)
this is just the Iwasawa decomposition into diagonal (we saw before) and q-deformed nilpotent (here just means lower left nonzero entry)
And they say "therefore as an algebra it has the structure
Func(H+q)= +IMat2I+1(C)
And they say "this description is the deformation of the foliation of H+ by quantum fuzzy spheres. Quantum fuzzy spheres have been introduced and studied in hep-th/0005273 (Grosse, Madore, Steinacker "Field Theory on the q-deformed Fuzzy Sphere")
At this point my outrage knows no bounds. But what can one do. The speeds that things were traveling at the instant the universe began to expand has according to good authority somewhat to do with q-deformed Fuzzy Spheres. Speeds were quantized. Oh damn the matrix looks the same but the entries are "non-commutative numbers". Oh hell it is awful. It looks like
except the n has been multiplied by something extremely close to one, namely
√((q2+1)/2)
you can see that since the deformation parameter is very close to one namely like
q = exp(-10-123) as it is today, then
this square-root thingee is very close to √(2/2) = 1
So the matrix Karim and Philippe (Noui/Roche) give us is
It seems likely that the next step in developing Covariant Loop Gravity will be a continuation of Livine's thesis that introduces positive Lambda----positive dark energy, or cosmological constant---into the theory.
The key new idea we need to grasp is that the "quantum hyperboloid becomes a stack of fuzzy spheres"
see first paragraph page 2 of Girelli/Livine "Quantizing Speeds with the Cosmological Constant" gr-qc/0311032
see also their equation (1)
The basis for "Quantizing Speeds..." is what now seems to be a very important paper by Karim Noui and Philippe Roche "Cosmological Deformation of Lorentzian Spin Foam Models" gr-qc/0211109
and in particular page 13 where the hyperboloid of possible speeds is put in terms of some 2x2 matrices---a right coset homog. space SU(2)\SL(2,C) and the Iwasawa decomposition is used to get it as A x N (diagonal and nilpotent) How bad can it be? It is just a few 2x2 matrices of especially simple form
lambda 0
0 lambda-1
plus
0 0
n 0
the first is the real number diagonal det=1 type
and the second is the complex number n for nilpotent
lower triangular type, the language here is heavier than the matrices
let's see if I can type the sum of those two matrices
Code:
[font=symbol]l[/font] 0
n [font=symbol]l[/font][sup]-1[/sup][/size]
so the hyperboloid of possible speeds, or moving observers, or boosts or whatever, is happily pictured algebraically as some 2x2 matrices
NOW Noui/Roche will tell us how to q-deform them by introducing a cosmological constant.
See page 16 and 17
You will see elegant french style. first the quantum hyperboloid is presented in a fearsomely succinct and categorical way, then in equation (55) one sees that it is simply a stack of spheres made of essemtially the same matrices except the lower left entry, the complex number n, has been multiplied by something EXTREMELY NEAR ONE.
and then presto on the next page there is equation (58) that Girelli and Livine used to see the spectrum of quantized speeds.
The fearsome and succinct definition they give first is something else. They refer to the algebra of compactly supported functions on the quantum hyperboloid as
Func(H+q) = Func(ANq)
this is just the Iwasawa decomposition into diagonal (we saw before) and q-deformed nilpotent (here just means lower left nonzero entry)
And they say "therefore as an algebra it has the structure
Func(H+q)= +IMat2I+1(C)
And they say "this description is the deformation of the foliation of H+ by quantum fuzzy spheres. Quantum fuzzy spheres have been introduced and studied in hep-th/0005273 (Grosse, Madore, Steinacker "Field Theory on the q-deformed Fuzzy Sphere")
At this point my outrage knows no bounds. But what can one do. The speeds that things were traveling at the instant the universe began to expand has according to good authority somewhat to do with q-deformed Fuzzy Spheres. Speeds were quantized. Oh damn the matrix looks the same but the entries are "non-commutative numbers". Oh hell it is awful. It looks like
Code:
[font=symbol]l[/font] 0
n [font=symbol]l[/font][sup]-1[/sup][/size]
√((q2+1)/2)
you can see that since the deformation parameter is very close to one namely like
q = exp(-10-123) as it is today, then
this square-root thingee is very close to √(2/2) = 1
So the matrix Karim and Philippe (Noui/Roche) give us is
Code:
[font=symbol]l[/font] 0
√((q[sup]2[/sup]+1)/2)n [font=symbol]l[/font][sup]-1[/sup][/size]
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