VIEW THIS AS

Auto mode follows the Route Engine until you choose a viewpoint.

YOU ARE HERE

ROUTE CHECK

CONNECTED TO

WHAT NEXT

Use the canonical route for this room, or HELP if you are unsure.

How Science Works | Matter-Wave Collapse and Revival — How Quantum Phases Reassemble

Three learners review open books together at a classroom table, with stacks of textbooks, stationery and a whiteboard in the bright room.

HOW SCIENCE WORKS · ATOMIC PHYSICS

Matter-Wave Collapse and Revival — How Quantum Phases Reassemble

A condensate’s interference pattern can fade and later return even while the system remains isolated. In a deep optical lattice, interactions make different atom-number components acquire different phases; their later realignment rebuilds the observable matter-wave coherence.

Choose a chapter · Atomic Physics hub

Find your reading route

Understand the mechanism · Chapters 1–2
  1. Coherence can disappear from an observable
  2. Number components accumulate different phases
Work through the prediction · Chapters 3–4
  1. Calculating the revival time
  2. Collapse is different from measurement reduction
Read the experiment and limits · Chapters 5–6
  1. The 2002 optical-lattice experiment
  2. Why real revivals decay

CHAPTER 1 OF 6

1. Coherence can disappear from an observable

Back to contents

A condensate loaded into an optical lattice occupies many wells. If their phases are coherent, releasing the atoms produces a sharp interference pattern. A rapid increase in lattice depth suppresses tunnelling and lets interactions within each well dominate.

After a suitable hold time, the interference peaks can weaken. This loss of visible contrast need not mean the atoms have disappeared or that every quantum correlation has been destroyed. The relevant question is how the state evolved before the image was taken.

Contents · Next chapter

CHAPTER 2 OF 6

2. Number components accumulate different phases

Back to contents

For an isolated lattice site with two-body interaction energy U, a simple Hamiltonian is H = U n(n−1)/2. A component containing n atoms acquires phase exp[−iUn(n−1)t/(2ℏ)].

An initial state with several occupied number components therefore develops a structured spread of relative phases. Their contributions to the mean matter-wave field stop adding constructively, and the interference contrast collapses.

Contents · Previous chapter · Next chapter

CHAPTER 3 OF 6

3. Calculating the revival time

Back to contents

In the ideal two-body model, the phases reassemble after trev = h/U. Because n(n−1) is always even for integer n, every number component returns to the same relative phase at that time.

If U/h = 800 Hz, the predicted revival time is 1/800 second = 1.25 ms. A lattice-depth scan changes U and should change the revival period accordingly. This illustrative calculation is a stronger test than simply noting that a contrast maximum returned once.

Experimental handlePhysical roleEvidence check
Interaction USets ideal revival periodTest trev = h/U
Initial number distributionControls collapse envelopeModel preparation statistics
Lattice homogeneityControls revival contrastCompare depth and trap gradients
How the controls connect the model to a measurable result.

Contents · Previous chapter · Next chapter

CHAPTER 4 OF 6

4. Collapse is different from measurement reduction

Back to contents

Here the word collapse describes the decay of a field expectation value or interference visibility under interaction-driven evolution. It is not a claim that a projective measurement has irreversibly selected one atom-number state.

The global state can remain coherent while the chosen first-order observable becomes small. A revival shows that some phase information remained in the dynamics. It does not imply that all apparent decoherence in other systems must be reversible.

Contents · Previous chapter · Next chapter

CHAPTER 5 OF 6

5. The 2002 optical-lattice experiment

Back to contents

Greiner and colleagues observed collapse and revival of a condensate’s matter-wave field in an optical lattice. Time-of-flight interference patterns revealed the disappearance and return of coherence after controlled hold times.

The primary result exposed the role of discrete atom number and interactions. A classical average-density treatment does not retain the same number-dependent phase structure, so the revival sequence probes a deeper description than a single smooth density profile.

Contents · Previous chapter · Next chapter

CHAPTER 6 OF 6

6. Why real revivals decay

Back to contents

Different wells can have different interaction strengths and occupancies. Residual tunnelling, external potential gradients, atom loss and effective higher-body terms can shift or wash out the revival pattern.

Researchers vary lattice depth, compare several revival periods, calibrate trap gradients and model the initial number distribution. The scientific lesson is that a missing signal can reflect dephasing among structured contributions; its controlled return can reveal the energy spectrum that organised them.

Primary research: Greiner and colleagues, Collapse and revival of the matter wave field of a Bose–Einstein condensate (Nature, 2002).

Continue through the Atomic Physics learning hub or the How Science Works master index.

Contents · Previous chapter · Atomic Physics hub

Discover more from eduKate Singapore

Subscribe now to keep reading and get access to the full archive.

Continue reading