Initial Question
How does a theory of quantum gravity contradict the Schrödinger equation?
Core Answer
The Schrödinger equation does not contradict a theory of quantum gravity per se; rather, it is fundamentally inadequate to describe a universe where spacetime itself is quantum and dynamical. The assumptions baked into the Schrödinger equation break down in the regimes where quantum gravity becomes important.
Detailed Breakdown of Conceptual Clashes
1. The Nature of Spacetime: Fixed vs. Dynamical
The Schrödinger Equation's Assumption: It treats time as a universal, absolute, and classical background parameter. The equation is:
Here, t is an external, smoothly flowing label against which quantum evolution is measured. Space is also a fixed, static stage.
General Relativity's Reality: In GR, spacetime is dynamic and interactive. It's not a stage but a flexible fabric that curves and evolves in response to matter and energy. There is no universal time; time is local and relative, woven into the spacetime metric.
The Contradiction/Incompatibility: A theory of quantum gravity aims to make this dynamical spacetime subject to quantum rules. But the Schrödinger equation requires a fixed, classical time to even be written down. What is 't' in the Schrödinger equation when time itself is a quantum variable that can fluctuate?
2. The Problem of Time
This is the most profound technical issue. In canonical approaches to quantum gravity (like the Wheeler-DeWitt equation), a fundamental constraint arises:
This is the Wheeler-DeWitt equation for the wavefunction of the universe |Ψ⟩. Notice the critical difference: there is no ∂/∂t.
This suggests that in a closed universe (with no external clock), the fundamental description is timeless. The wavefunction of the universe describes correlations between physical variables, but not evolution in an external time. How to recover the familiar flow of time from this timeless equation is a major puzzle, known as the "Problem of Time." The Schrödinger equation, with its explicit time dependence, simply doesn't emerge naturally at this fundamental level.
3. Unitarity vs. Black Hole Information Paradox
The Schrödinger equation guarantees unitarity: the total probability is conserved over time. This is a cornerstone of quantum mechanics.
Black Hole Evaporation (Hawking Radiation): In a semi-classical treatment, black holes evaporate and appear to destroy information (pure states evolve into mixed states), which violates unitarity.
Quantum Gravity's Task: A full theory of quantum gravity must resolve this paradox. It must either preserve unitarity (showing information escapes) or fundamentally modify quantum mechanics to allow for non-unitary evolution. Either outcome challenges the applicability of the standard Schrödinger framework in extreme gravitational settings.
4. Quantum Superposition of Spacetime Geometries
In quantum gravity, spacetime itself should be able to exist in superpositions (e.g., a superposition of different curvatures or topologies). The Schrödinger equation evolves a quantum state on a spacetime. It has no machinery to describe a quantum state of spacetime.
Summary & Synthesis
Think of it like Newton's laws and special relativity. Newton's laws aren't "wrong" in a limited domain, but they are built on assumptions (absolute time and space) that break down at high speeds. You don't contradict F=ma; you subsume it into a more fundamental framework.
The key insight: The Schrödinger equation is an extremely successful approximation for quantum physics on a fixed, classical spacetime background. A theory of quantum gravity is needed to describe physics where the spacetime background is itself quantum and dynamical.
How Proposed Frameworks Tackle This
String Theory: The Schrödinger equation emerges as an effective, low-energy approximation. Fundamental objects are strings propagating in a background, but the framework aims to be background-independent in principle.
Loop Quantum Gravity: Works directly in a background-independent manner. The Wheeler-DeWitt-like constraint (Ĥ |Ψ⟩ = 0) is central, and time must be recovered from within the system.
Causal Set Theory & Others: Also start from fundamentally discrete, background-free principles.
Final Conclusion: The Schrödinger equation isn't contradicted point-by-point; it's rendered inapplicable because its core prerequisite—a fixed, classical time parameter—is absent in the regime where gravity and quantum mechanics are inseparable. The quest for quantum gravity is, in part, the quest to find the more general equation of which the Schrödinger equation is a limiting case.