The Mystery of Time in Physics
Exploring the complex relationship between time and timeless theories in physics.
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In the world of physics, especially in the study of gravity and quantum mechanics, there is a curious idea that time might not be as straightforward as we believe. Some theories suggest that time is not a basic part of the universe but instead comes from something that is fundamentally timeless. This belief leads to various challenges when trying to understand how time arises in these theories.
One common approach in understanding gravity is known as quantum gravity. This field tries to combine general relativity, which explains gravity, with quantum mechanics, which deals with very small particles. Many scientists suggest that time appears after we make certain simplifications or approximations in these theories. However, this raises an important question: what allows us to make these approximations in the first place? When we look deeper, it seems that the concept of time sneaks back into the picture, creating worry about whether we are genuinely deriving time from a timeless nature or if we are being circular in our thinking.
In our everyday lives, we see change and experience time as a progression. But in some scientific models, the starting point is a kind of physics that does not include time at all. This creates a paradox. If we want to say that time comes from timeless physics, but the process of arriving at this conclusion seems to require time, then the reasoning appears flawed. It's as if we are trying to define time while assuming it already exists.
When scientists look at the problem of time, they often refer to an approach called the semiclassical time program. This program suggests that time can emerge from timeless settings when we focus on the right approximations. However, if we scrutinize these approximations, we find that they may rely on time-related justifications. This leads us to wonder if the entire framework we are using to describe time might be incorrect.
The Semiclassical Time Program
The semiclassical time program is one of the oldest frameworks scientists use to understand how time might emerge in quantum mechanics. It involves breaking down spacetime into different parts, where one part represents the three dimensions of space and the other part deals with time. In this setup, the gravitational fields, which we think of as representing gravity, are treated as if they can independently contribute to time.
This program suggests that when we apply certain mathematical techniques, we can derive a version of time even if we start from a situation where time isn’t directly included. The equations used in this approach show how correlations between different elements might behave as if they are changing over time. However, a critical issue arises when we try to justify the assumptions we make to reach these equations.
The Need for Observers
A key part of understanding how measurements work in physics is the role of observers. Observers allow us to get a sense of what we consider "small" or "large" in a physical system. In quantum gravity, however, we lack a clear idea of what an observer is within this timeless setting. Without observers, we cannot gauge whether certain changes in our equations are significant or not.
For example, when using the semiclassical program to derive time, we often rely on approximations that seem reasonable. These approximations assert that one part of the system behaves independently over time. However, to justifiably claim this independence, we need a means to measure small differences, which requires an observer. Yet, if we introduce observers into the discussion, we are already assuming the existence of time, leading to circular reasoning.
Approximation Techniques
The semiclassical time program often relies on a few key approximation methods, which initially appear to be grounded in simple physical reasoning. The first method is called the Born-Oppenheimer Approximation. This technique is based on the idea that there are different scales of mass in the universe. When one part has much larger mass than another, it might change slowly relative to the lighter part. This allows scientists to treat the heavier mass as if it is essentially static over short timescales.
While this justification sounds reasonable, it inherently invokes concepts of time. The differences in mass don't explain themselves without reference to how these masses interact over time. If we want to consider changes in a system, we must factor in the time over which those changes happen.
Another commonly used method is the WKB Approximation. This mathematical technique is used in various fields of quantum mechanics, particularly when dealing with stationary states of energy. The trick here is that this method presumes a certain smoothness in the potential landscape of the system, indicating that something is changing slowly over time. Implicitly, it assumes some background time metric that allows us to say the changes are insignificant over short periods. Therefore, the use of WKB also brings in concerns about time, even while it aims to derive it formally.
The Role of Decoherence
Decoherence is another concept that comes into play when discussing how systems reach certain states. In quantum mechanics, if a system is in an entirely mixed state, decoherence helps convert that state into a mixture of non-interacting components. This process usually hinges on some form of temporal evolution - a characteristic that inherently depends on time.
When referencing decoherence as a justification within the semiclassical time program, we face yet another issue. The requirements for decoherence present a tension since the act of decohering involves time. Thus, if decoherence is necessary for the emergence of time, we encounter a paradox: we cannot justify the presence of time without assuming time.
The Circular Reasoning
In summary, the semiclassical time program seemingly requires us to introduce concepts of time to derive time from a foundation that claims to be timeless. This leads us to a dilemma: can we truly derive a notion of time from an approach that explicitly tries to exclude it? The various approximations used in the program, such as the Born-Oppenheimer method, the WKB approximation, and decoherence, all rely on time to justify their existence.
Hence, instead of providing a clear perspective on how time might arise, the semiclassical time program raises critical questions about its validity. We observe that the assumptions made are not neutral; they appear to carry hidden notions of time. So, while the theory suggests a view of the universe as fundamentally timeless, it ultimately asks us to don "time glasses" to make sense of its findings, thereby reaffirming time's presence in the process.
The questions about how time emerges from this timeless construct force a reconsideration of not just the methods we use but also the foundations of the theories at play. This inquiry may lead us to realize that instead of illuminating our understanding of time, these approaches could be clouding our vision by mixing time with timeless assertions. The search for an unambiguous understanding of time continues, as we attempt to resolve these intricate challenges at the intersection of gravity and quantum mechanics.
Title: No Time for Time from No-Time
Abstract: Programs in quantum gravity often claim that time emerges from fundamentally timeless physics. In the semiclassical time program time arises only after approximations are taken. Here we ask what justifies taking these approximations and show that time seems to sneak in when answering this question. This raises the worry that the approach is either unjustified or circular in deriving time from no-time.
Authors: Eugene Y. S. Chua, Craig Callender
Last Update: 2023-03-26 00:00:00
Language: English
Source URL: https://arxiv.org/abs/2303.14854
Source PDF: https://arxiv.org/pdf/2303.14854
Licence: https://creativecommons.org/licenses/by/4.0/
Changes: This summary was created with assistance from AI and may have inaccuracies. For accurate information, please refer to the original source documents linked here.
Thank you to arxiv for use of its open access interoperability.