ivan said:
What I meant was there's no objective description of time since there's no unitary idea of time in physics, or different parts of physics.
You are absolutely right that different definitions of time in different parts of physics (e.g., in quantum mechanics and in special relativity) cannot be tolerated. There should be a unique definition of time across all physics. I suggest that quantum-mechanical definition (time as a classical parameter of reference frames) should be used.
ivan said:
I want to clarify this for me. If I'm mistaken please correct me. When we say position is an 'observable' we probably mean that a particle's (or macroscopic object's) position can be observed. Observation can be performed through a 'naked' eye or some type of measuring device like florescent screen that can light up when particle hits it.
You've mentioned Hermitian operator. I do not know that much math. So, when I talk about observing a position of a something I mean I could sea what you (as a physicist) could see physically in a given experiment. You describe observation in a certain abstract way to make physics meaningful, though finally it all comes to observing things through vision or hearing (whether seeing a flash or hearing a click).
Yes, you are basically correct.
It is important to understand that theoretical physics is not supposed to give us a comprehensive picture of the world. Its role is more modest: it must describe and predict results of measurements performed in well-controlled experimental setups. When you perform an experiment you usually have a pretty good idea about what is the observed physical system (atom, molecule, crystal, rock, planet, etc.), what is the measuring apparatus (bubble chamber, Geiger counter, ruler, telescope, etc.), and what constitutes the "measurement" (flash, click, blackening of the photographic plate). If a theory can predict exactly (the probabilities of) these flashes and clicks, then the role of theory is fulfilled.
Each observer (or reference frame) should have one specific device called "clock". When observer performs a measurement he also looks at the clock reading and assigns a label "time" to the measurement. This label does not depend on what physical system was observed and what physical property of the system was probed. In this respect "time" is very different from other "observables", such as position, momentum, spin, energy, etc. which are intimately related to the observed physical system and its state.
ivan said:
This is not quite clear to me. By 'no phycial system' I guess you mean no physical system other than the clock. Since I think the clock also presents the physical system which we observe. This might include the observation of the positions of the clock's arms.
This depends on you experimental setup. Yes, you may decide to treat the clock as your physical system and treat the position of the clock's arm as the observable. Then the clock is no longer a measuring device (i.e., not a part of the reference frame), but the observed physical system. In this case you should use some other device as a clock (i.e., for generating time labels of measurements) in your reference frame. The bottomline is that in experiment you must always have a clock which is not a part of your observed system, but a part of your measuring setup.
Eugene.