The Role of Time in Physics: Exploring Traces from the Past and Future

In summary: However, in special relativity, Maxwell's equations \frac{\partial E}{\partial t} = \frac{\partial P}{\partial x} = 0 (3)are nonlinear. Therefore, the space-time continuum cannot be transformed into the Lorentz manifold, and vice versa.Second, the space-time continuum is not compact. If it were, then the curvature of spacetime would cause a distortion of the trajectories of particles, violating the principle of relativity.Third, the space-time continuum is not static. If it were, then the gravitational field would cause a distortion of the space-time continuum, violating the principle of
  • #1
surena1980
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0
The Time is not a ket nor an operator, so what role does the Time play in Physics?
 
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  • #4
Sakurai calles it a "parameter" (without a proper definition, but that's Sakurai). Also see https://www.physicsforums.com/showthread.php?t=136126 .
 
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  • #5
Dmtr, thanks for the links. It seems very interesting.
 
  • #7
There can be no "operator of time" in quantum mechanics. Suppose there is such an operator [tex]T[/tex]. Then, there it should possesses mutually orthogonal eigenvectors [tex]|t \rangle [/tex] with eigenvalues [tex]t[/tex]. However, the state represented by the eigenvector [tex]|t \rangle [/tex] is physically impossible. In this state particle exists only in a short time interval around [tex]t[/tex]. Such a state violates all existing conservation laws.

So, time is not an observable. Time is not a property or attribute of a physical system. Time is rather an attribute of the measuring device or observer. When we measure certain true observable (position, spin, etc) we attach a label (time) to this measurement in accordance with what the laboratory clock showed at the instant of measurement. So, mathematically it is OK to treat time as a numerical parameter, as it is done in ordinary quantum mechanics.

Also I think that it is not useful to demand that time and space should be treated on "equal footing". Space-time unification is not an essential feature of relativistic physics. The true postulates of relativity are: (1) all inertial reference frames are equivalent (2) the group of transformations between inertial reference frames is the Poincare group. In QM this implies that the Hilbert space of any isolated physical system carries an unitary representation of the Poincare group. This is the true and complete mathematical manifestation of the principle of relativity. The "symmetry" between space and time is an additional unjustified assumption.

Edit: for more details see

E. V. Stefanovich, "Is Minkowski space-time compatible with quantum mechanics?", Found. Phys., 32 (2002), 673.

Eugene.
 
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  • #8
Time is linked to energy on QM though, but that is if you assign any credibility to the "weak" uncertainty of time and energy and since the relation is non-commutative and yields a constant it must be an operator. How else could information of correlated spins between two “particles” be transferred instantaneously if time isn’t an operator?

Just looked at a john Baez site and he gives a compelling reason that time is not an operator. I still think it is and by not coming to terms with it may be missing some great discoveries in QM.


I may be wrong? I took a turn out of math and physics and went to the horrible world of economics, econophysics and finance.
 
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  • #9
statespace101 said:
Time is linked to energy on QM though, but that is if you assign any credibility to the "weak" uncertainty of time and energy and since the relation is non-commutative and yields a constant it must be an operator.

Yes, there is the time-energy uncertainty relationship. The primary example is an unstable particle, whose lifetime is inversely proportional to the energy (mass) uncertainty. However, the nature of this relationship is completely different from the position-momentum uncertainty relationship (where two non-commuting operators are involved). Particle decays with all their features can be described pretty well in ordinary quantum mechanics, where time is not an operator.

Eugene.
 
  • #10
The link dmtr posted by just reading the beginning made me realize that time must be an operator for the delyaed choice quantum eraser to be possible. I looked at John von's memory space and that just clicked.

Or how about Wigner's friend, Eugene? Just kidding Wigner Eugene Wigner irony :lol:
 
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  • #11
meopemuk said:
Also I think that it is not useful to demand that time and space should be treated on "equal footing". Space-time unification is not an essential feature of relativistic physics.

We may never make satasfactory progress in QM until we respect Special Relativity. This means, of course, that we must regard the notion of 'time' as 'spacetime,' whether in cosmology or QM.
 
  • #12
Another good example I just posted in another thread is the Aharonov-Bohm effect. That time is an operator, or you believe it's a hidden variable. Ballentine goes over this in his book, Quantum Mechanics: A Modern Development by Leslie E. Ballentine.
 
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  • #13
Neo_Anderson said:
We may never make satasfactory progress in QM until we respect Special Relativity. This means, of course, that we must regard the notion of 'time' as 'spacetime,' whether in cosmology or QM.

Let us suppose that you are right and that space and time are unified in a 4-dimensional continuum. I would like to show that this assumption leads to a contradiction with other important postulates of relativity and quantum mechanics.

First, the space-time idea is equivalent to the assumption that Lorentz transformations

[tex] x' = \frac{x-vt} {\sqrt{1-v^2/c^2}} [/tex]......(1)
[tex] t' = \frac{t -vx/c^2} {\sqrt{1-v^2/c^2}} [/tex]...(2)

are exact and universal. For example, if [tex]x, x'[/tex] are particle positions in different frames, then the above transformations are true independent on whether this particle is free or it is a part of an interacting multiparticle system. The transformations do not depend on the strength of this interaction as well.

Now, let me look at these transformations from another perspective. In relativistic quantum mechanics a multiparticle system is described in the Hilbert space, in which a unitary representation of the Poincare group is defined. If the system is interacting then, as it is well-known, the generator of time translations (the Hamiltonian [tex]H[/tex]) is interaction-dependent (i.e., it is different from the free-particle form). It is less-known that the vector of boost generators [tex]\mathbf{K}[/tex] must be interaction-dependent too (you can read more about that in S. Weinberg's "The quantum theory of fields", vol. 1). The boost generator is exactly what we need to find out how particle position operators [tex]X,X'[/tex] are related to each other in relatively moving reference frames. If the movement is along the x-axis with rapidity [tex]\theta[/tex], then the QM formula is

[tex]X' =\exp(-iK_x \theta)X\exp(iK_x \theta) [/tex].....(3)

Since operator [tex]K_x[/tex] is interaction-dependent, the transformation (3) must have different forms depending on the nature of the multiparticle system and on interactions acting there. This conclusion is in direct contradiction with the exactness and universality of (1) assumed earlier.

Eugene.
 
  • #15
Demystifier said:
I have written a comment on it:
http://xxx.lanl.gov/abs/0912.1947

then an entropy-decreasing transformation leaves a
trace from the future. Yet, in nature we do not see traces
from the future and the results of [1] do not explain why.

Are you assuming a single history line? In the MWI you are going to have contributions from all possible futures, I guess they will destructively interfere / cancel out.
 
  • #16
dmtr said:
Are you assuming a single history line? In the MWI you are going to have contributions from all possible futures, I guess they will destructively interfere / cancel out.
Well, I have written a comment on a particular paper which does not use MWI.
In the spirit of this comment, I would object to you that you don't explain why only futures cancel out and not the pasts.

In a more general (not related to the criticized paper) MWI context, I object to you that different MACROSCOPIC histories do not interfere due to decoherence.
 
  • #18
Paper: http://arxiv.org/abs/0802.0438
Criticism: http://xxx.lanl.gov/abs/0912.1947

Demystifier said:
Well, I have written a comment on a particular paper which does not use MWI. In the spirit of this comment, I would object to you that you don't explain why only futures cancel out and not the pasts.

IMHO a good theory (or criticism) should hold under any QM interpretation (as QM interpretations do not change the underlying equations, they are essentially the ways to visualize different aspects of the equations). The original article didn't use the term 'single, well defined future', you did. That's why I've tried to apply MWI and show that your criticism about the traces from the future is not a very sound one.

As far as the original goes about the 'traces from the future' - the author says that we will consider these traces to be from the past:

In addition, I recall that there is a substantial problem
in rigorously defining past and future without resorting
to the second law (which would then be reduced to a
mere definition). In fact, the laws of physics are time-
reversal invariant. Hence, there is no preferred direction
of time according to which we may establish a substantial
difference between the two temporal directions past-to-
future and future-to-past [37]. Anthropocentrically, we
could define the past as that of which we have memories
of, and the future as that of which we do not have any
memories. Of course, such definition cannot be made rig-
orous, since it resorts to a observers and their memories.
However, even using this ambiguous, intuitive definition
of past, it is clear that any event, which cannot have any
correlation with us, does not pertain to our past just as
if it had never happened.
 
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  • #20
dmtr said:
IMHO a good theory (or criticism) should hold under any QM interpretation (as QM interpretations do not change the underlying equations, they are essentially the ways to visualize different aspects of the equations). The original article didn't use the term 'single, well defined future', you did. That's why I've tried to apply MWI and show that your criticism about the traces from the future is not a very sound one.
Perhaps the original article didn't use the term "single, well defined future", but it used "single, well defined past" and "symmetry between the two time directions", which, taken together, imply "single, well defined future". That is my point. It does not depend on the interpretation of QM.
 
  • #21
dmtr said:
As far as the original goes about the 'traces from the future' - the author says that we will consider these traces to be from the past:
Since he does NOT EXPLAIN why not to consider traces from the future, he has not right to say that he can explain the origin of the arrow of time. Yet, he claims that. And that's the basis of my criticism.
 

FAQ: The Role of Time in Physics: Exploring Traces from the Past and Future

What is the concept of time in physics?

In physics, time is considered to be a fundamental quantity that helps us measure the duration or sequence of events. It is defined as the progression of events from the past to the present and into the future.

How does time relate to the laws of physics?

Time plays a crucial role in the laws of physics, as it is a fundamental component in the equations that govern the behavior of matter and energy. For example, the concept of time dilation in Einstein's theory of relativity explains how time can appear to pass differently for objects that are moving at different speeds.

What is the connection between time and space in physics?

In physics, space and time are often considered together as "spacetime." This is because the laws of physics are described in terms of both space and time, and they are intertwined in the fabric of the universe. Einstein's theory of general relativity describes how the presence of mass and energy can warp the fabric of spacetime, affecting the passage of time.

Can time be manipulated or controlled in physics?

While time travel and manipulation of time may be popular concepts in science fiction, in physics, time is considered to be a constant and unchangeable quantity. However, the rate at which time passes can be affected by factors such as gravity and velocity, as explained by the theory of relativity.

What are some ongoing research and theories about time in physics?

There are many ongoing research and theories about time in physics, including the search for a unified theory that can reconcile the discrepancies between Einstein's theory of relativity and quantum mechanics. Other areas of interest include the concept of "arrow of time" and the possibility of parallel universes with different timelines.

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