- #36
cianfa72
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Ok thanks, now it makes sense.PeterDonis said:I see that I did incorrectly use "coordinate speed" later on in that post. I have edited it to correct those statements.
Ok thanks, now it makes sense.PeterDonis said:I see that I did incorrectly use "coordinate speed" later on in that post. I have edited it to correct those statements.
I think it is mathematically described from the FLRW metric that on spacelike hypersurfaces of constant cosmological time ##t## is homogeneous and isotropic.PeterDonis said:More precisely, as an example, every such observer would measure the CMB to have the same temperature in all directions. That is an indication that the universe is seen to be isotropic. And if we pick out one particular spacelike hypersurface, at the event on each such worldline that is in that hypersurface, each observer would measure the CMB temperature to have the same numerical value. That is an indication that the universe is seen to be homogeneous.
No, it isn't; that doesn't even make sense.cianfa72 said:I think it is mathematically described from the FLRW metric that on spacelike hypersurfaces of constant cosmological time ##t## is homogeneous and isotropic.
It doesn't make any sense to say that a metric (restricted on spacelike hypersurfaces) is homogeneous and isotropic ?PeterDonis said:No, it isn't; that doesn't even make sense.
I thought your post #37 was saying that ##t## (the coordinate) is homogeneous and isotropic. That doesn't make sense.cianfa72 said:It doesn't make sense to say that a metric (restricted on spacelike hypersurfaces) is homogeneous and isotropic ?
From a mathematical point of view, the homogeneous property of a Riemannian manifold (that is any spacelike hypersurface of constant cosmological time) boils down to the existence of a transitive isometry map on it.PeterDonis said:It makes sense to say that the geometry of a spacelike hypersurface of constant ##t## is homogeneous and isotropic, so if by "metric" you mean "geometry" then it would also make sense to say the metric is homogeneous and isotropic.
Yes.cianfa72 said:From a mathematical point of view, the homogeneous property of a Riemannian manifold (that is any spacelike hypersurface of constant cosmological time) boils down to the existence of a transitive isometry map on it.
It means that, if we pick a point in the manifold, there is an SO(3) isometry centered on that point.cianfa72 said:What about the mathematical definition of isotropic for that manifold ?
SO(3) is the special continuous group of linear transformations that preserves orthogonality. In this context the orthogonality is w.r.t. the (positive definite) metric tensor defined on each point on spacelike hypersurfaces.PeterDonis said:It means that, if we pick a point in the manifold, there is an SO(3) isometry centered on that point.
SO(3) is the group of rotations in 3 dimensional space. These are linear transformations and they do preserve the orthogonality, but they are hardly the only such group of transformations. So I don't see where you are getting "the" (bolded in the quote above) from.cianfa72 said:SO(3) is the special continuous group of linear transformations that preserves orthogonality.
Yes.cianfa72 said:An element of SO(3) group acts on vectors of tangent vector space defined at each point.
That's what I said.cianfa72 said:Therefore, I think, the definition of isotropy at a point does require SO(3) group elements act on tangent space's vectors as isometries.
Note that, while this is correct, it is not the only possible way to interpret the SO(3) group. It can also be interpreted as a three-parameter group of Killing vector fields on the spacetime. A spacetime with such a group of KVFs is called "spherically symmetric", and will be isotropic about at least one point, but possibly only one. For example, a spacetime containing a single non-rotating body surrounded by vacuum will be spherically symmetric, and will be isotropic about the center of mass of the body, but not about any other point.cianfa72 said:An element of SO(3) group acts on vectors of tangent vector space defined at each point.
Ok, so you are saying that there could be other groups of possibly non-linear transformations that preserve orthogonality and length as well.PeterDonis said:SO(3) is the group of rotations in 3 dimensional space. These are linear transformations and they do preserve the orthogonality, but they are hardly the only such group of transformations. So I don't see where you are getting "the" (bolded in the quote above) from.
Ok, so integral curves of such KVFs lie on spacelike hypersurfaces, I believe.PeterDonis said:Note that, while this is correct, it is not the only possible way to interpret the SO(3) group. It can also be interpreted as a three-parameter group of Killing vector fields on the spacetime. A spacetime with such a group of KVFs is called "spherically symmetric", and will be isotropic about at least one point, but possibly only one.
... or groups of linear transformations that do preserve orthogonality but don't preserve lengthcianfa72 said:there could be other group of possibly non-linear transformations that preserve orthogonality and length as well
They lie within each spacelike hypersurface of constant FRW coordinate time.cianfa72 said:integral curves of such KVFs lie on spacelike hypersurfaces, I believe.
Yes. But we can also consider points in a spacelike hypersurface of constant FRW coordinate time, since the integral curves of the KVFs in question like entirely within such surfaces.cianfa72 said:when you say "point" you are actually mean an event in spacetime.
That means the three-parameters family of KVFs (that form a Lie algebra) are the infinitesimal generators of a group of isometries centered on any point on each spacelike hypersurface of constant cosmological time. Such groups are different instances each isomorphic to SO(3).PeterDonis said:In the case of FRW spacetime, however, the spacetime is isotropic about every point. That means it is spherically symmetric no matter which point we choose as our center of symmetry. It also means that there is a different SO(3) group of KVFs centered on each such point. In other words, a much stronger set of properties than just an SO(3) isometry on tangent spaces.
Of SO(3) KVFs, yes. Note that the isometries associated with homogeneity, the spatial translations in a spacelike hypersurface of constant time, are also generated by a three-parameter group of KVFs, but the group is not SO(3).cianfa72 said:the three-parameters family of KVFs (that form a Lie algebra) are the infinitesimal generators of a group of isometries centered on any point on each spacelike hypersurface of constant cosmological time.
I guess you could think of them that way, although I don't think the term "instances" appears in this connection in the literature.cianfa72 said:Such groups are different instances each isomorphic to SO(3).
Sorry, such KVFs form a Lie algebra (w.r.t. the Lie bracket). Are themselves elements of SO(3) group, or are the isometries they generate actually elements of groups each isomorphic to SO(3) ?PeterDonis said:Of SO(3) KVFs, yes. Note that the isometries associated with homogeneity, the spatial translations in a spacelike hypersurface of constant time, are also generated by a three-parameter group of KVFs, but the group is not SO(3).
Sure, any group of KVFs forms a Lie algebra.cianfa72 said:such KVFs form a Lie algebra
A Lie algebra is not the same as a Lie group. Elements of a Lie algebra can be generators of a Lie group.cianfa72 said:Are themselves elements of SO(3) group
It would be really helpful if you would be specific about which isometries you are talking about.cianfa72 said:or are the isometries they generate actually elements of groups each isomorphic to SO(3) ?
Yes, so the "set" of three-parameters KVFs associated with the isotropy at every point (on any spacelike hypersurface of constant FRW coordinate time) form a Lie algebra and generate isometries that form a Lie group isomorphic to SO(3).PeterDonis said:A Lie algebra is not the same as a Lie group. Elements of a Lie algebra can be generators of a Lie group.
Yes, I was referring to this three-parameter group.PeterDonis said:One three-parameter group, the one associated with isotropy at every point, is associated with the group SO(3).
Yes.cianfa72 said:We said FRW spacetime is spherically symmetric regardless the point we choose as center of symmetry.
Yes.cianfa72 said:The geometry of any spacelike hypersurface of constant cosmological time can be only one of the three type: flat (Euclidean), hyperbolic, spherical.
Yes.cianfa72 said:In any case there will be 6 linearly independent KVFs (one three-parameters "set" of KVFs for translations and one three--parameter "set" of KVFs for rotations about one chosen point).
I'm not sure what you mean by this. "Linearly independent" means that none of the KVFs can be expressed as a linear combination of the others.cianfa72 said:The notion of linearly independent KVFs actually means that all the coefficients of their linear combination that give the null vector field are null (zero).
No, this is not correct. A linear combination of a translation and a rotation is not a rotation about a different point.cianfa72 said:Now each other "set" of KVFs that are generators of the isometry group of rotations about any other point on that manifold can be given as linear combination of the first 6 KVFs. In other words, from the three-parameters translational KVFs and from the "set" of three-parameters rotational KVFs about one point, we get the set of three-parameters rotational KVFs about any other point.
I think I misinterpreted it. The set of KVFs on a manifold is not a vector space, therefore we can't get for instance a KVF for rotation about a different point as linear combination of overall 6 translation KVFs and rotation KVFs at another point.PeterDonis said:No, this is not correct. A linear combination of a translation and a rotation is not a rotation about a different point.
Maybe the result is the same as Lie dragging the rotation KVFs at one point along the integral curves of translation to another point.PeterDonis said:What is correct is that you can Fermi-Walker transport the "rotation" KVFs at one point along the integral curves of a translation to another point, and you will get the "rotation" KVFs at the other point.
Correct.cianfa72 said:The set of KVFs on a manifold is not a vector space
Actually, Lie dragging might be the correct transport law here. I believe we had a previous thread where we showed that Lie transport and Fermi-Walker transport are not necessarily the same.cianfa72 said:Maybe the result is the same as Lie dragging the rotation KVFs at one point along the integral curves of translation to another point.
I've some doubts about this. From the above 7 KVFs are not linearly independent (see also Sean Carroll Spacetime and geometry - section 3.9).cianfa72 said:The set of KVFs on a manifold is not a vector space, therefore we can't get for instance a KVF for rotation about a different point as linear combination of overall 6 translation KVFs and rotation KVFs at another point.
This definition should be equivalent to the existence of spacelike KVFs associated to those isometries (the pushforward is actually the differential of the isometry map evaluated at the point ##p##).More formally, a manifold ##M## is isotropic around a point ##p## if, for any two vectors ##V## and ##W## in ##T_pM## there is an isometry of ##M## such that the pushforward of ##W## under the isometry is parallel with ##V## (not pushed forward).
More precisely, you can't find 7 linearly independent KVFs at a particular point in one spacelike hypersurface of constant FRW coordinate time. You can only find 6.cianfa72 said:7 KVFs are not linearly independent
A vector space is defined as a space satisfying a particular set of axioms. Look up those axioms and then check whether the set of KVFs on a manifold satisfies them.cianfa72 said:What does it mean ? We said that the set of KVFs on a manifold is not a vector space
If you are talking about linearly independent, look up the definition of that. That definition is not in terms of "some kind of operations". There is one particular operation involved. Look it up and see.cianfa72 said:Perhaps the point is that if we take 7 KVFs then we can always write down any of them by "some kind of operations" acting on the other 6 KVFs
This has nothing to do with either linear independence or forming a vector space. (Which are two different things, btw.)cianfa72 said:we get the rotation KFV about a point by Lie dragging the rotation KVFs about a different point.
Yes.cianfa72 said:This definition should be equivalent to the existence of spacelike KVFs associated to those isometries
Ah ok, so the the notion of linearly independence applies to KVFs "evaluated" at specific points.PeterDonis said:More precisely, you can't find 7 linearly independent KVFs at a particular point in one spacelike hypersurface of constant FRW coordinate time. You can only find 6.
Re-thinking about it, I believe the set of KVFs on a manifold is a real vector space. Namely the pointwise sum of two KVFs is a KFV (i.e. the sum is closed) as the scalar moltiplication for a real number (together with the Lie bracket such vector space is promoted to an algebra).PeterDonis said:A vector space is defined as a space satisfying a particular set of axioms. Look up those axioms and then check whether the set of KVFs on a manifold satisfies them.
No, it applies to vector fields in general. The reason I said "at a specific point" is that the KVFs associated with isotropy at different points are different KVFs.cianfa72 said:the notion of linearly independence applies to KVFs "evaluated" at specific points.
Those aren't the only vector space axioms.cianfa72 said:Re-thinking about it, I believe the set of KVFs on a manifold is a real vector space. Namely the pointwise sum of two KVFs is a KFV (i.e. the sum is closed) as the scalar moltiplication for a real number (together with the Lie bracket such vector space is promoted to an algebra).
I could be wrong but an algebra requires an underlying structure of vector space on a field -- Lie algebra.PeterDonis said:Those aren't the only vector space axioms.
That is true, but irrelevant to what I said.cianfa72 said:I could be wrong but an algebra requires an underlying structure of vector space on a field -- Lie algebra.
Sorry, I don't understand. If the set of KVFs on a manifold is a Lie algebra then it is a vector space on ##\mathbb R## w.r.t. the pointwise sum of KVFs.PeterDonis said:That is true, but irrelevant to what I said.
Ah, I see. Yes, that's correct.cianfa72 said:If the set of KVFs on a manifold is a Lie algebra then it is a vector space
My point is the following: start by noting that vector fields on a manifold form themselves a vector space on ##\mathbb R##, therefore it suffices to show that KVFs are closed both w.r.t. the vector field sum and the product for a scalar in ##\mathbb R##.PeterDonis said:However, I still think it would be a good idea for you to check that the set of KVFs satisfies all of the vector space axioms, not just the ones you mentioned.
No, it doesn't. You also have to show that the identity element of the vector space is in the set of KVFs. That might seem trivial, but it at the very least should give some food for thought.cianfa72 said:vector fields on a manifold form themselves a vector space on ##\mathbb R##, therefore it suffices to show that KVFs are closed both w.r.t. the vector field sum and the product for a scalar in ##\mathbb R##.
Yes, the identity element of the vector field vector space is the null vector field ##0##. If we "insert" it into post#68 definition we get $$\nabla_Y0 =0, \nabla_Z0=0,\ \forall Y,Z\in\Gamma(TM)$$ hence $$g(0,Z)=0, g(Y,0), \ \forall Y,Z \in\Gamma(TM)$$PeterDonis said:No, it doesn't. You also have to show that the identity element of the vector space is in the set of KVFs. That might seem trivial, but it at the very least should give some food for thought.