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Why Does Quantum Mechanics Use a Complex Wavefunction? Schrödinger’s equation doesn’t start from mystery. It starts from a very specific bet. The state of a particle is a complex field ψ(x,t), and whatever time-evolution rule we choose has to move ψ forward while preserving total probability. So the basic...

20,911 次观看 • 8 个月前 •via X (Twitter)

35 条评论

ItsBS 的头像
ItsBS8 个月前

Re: "Schrödinger’s equation doesn’t start from mystery. It starts from a very specific bet. The state of a particle" No. It doesn't start from the state of a particle. Particles are not involved with Schrodinger's Equation. Particles ideas are with Born's ad-hoc REDEFINITION

john vega Phd. science 的头像
john vega Phd. science8 个月前

This point of view forget negative part of scheme and (Y;Z) to be in 3D

Yukihiro Watanabe JP 的头像
Yukihiro Watanabe JP8 个月前

ψ^-^ψ

Jonathan D. Pratt, Ph.D. 的头像
Jonathan D. Pratt, Ph.D.8 个月前

This reminded me about the different convergence rates of the e series compared to the pi series: Here's Grok's summary: "For the volume formula itself: V = (4/3) π r³ = e^{ln(4/3)} π r³. Series for eˣ (and thus the 4/3 factor) The Taylor series for eˣ is eˣ = ∑_{n=0}^∞ (xⁿ / n!). This converges extremely quickly for finite x due to the factorial denominator growing faster than any exponential numerator. For this case: ln(4/3) ≈ 0.28768, so we're expanding e^{0.28768}. After just 5 terms: 1 + 0.28768 + (0.28768)²/2 + (0.28768)³/6 + (0.28768)⁴/24 ≈ 1.33333 (already spot-on to 5 decimals for 4/3 ≈ 1.33333). By 10 terms, it's precise to machine epsilon for most purposes. The series "settles" almost immediately, like a sprinter finishing the race before the crowd has sat down. Series for π Now contrast with π, which doesn't have a built-in fast-converging series like eˣ. The classic Leibniz formula is π = 4 ∑_{n=0}^∞ [(-1)ⁿ / (2n+1)]:First term: 4 (way off). After 10 terms: ≈ 3.04184 (error ~0.1). After 100 terms: ≈ 3.13159 (error ~0.01). It takes about 10⁶ terms for 6 decimal places—glacially slow, like a marathon runner who's still warming up after the e series has long finished."

Ron Messick 的头像
Ron Messick8 个月前

Here's my 2-cents: How the Complex Wavefunction Theorem Relates to Temporal Scalar Field Theory (TSFT) Your theorem explains why quantum mechanics must use a complex wavefunction: • The magnitude r(xⓜ,t) gives a conserved density r^2=∣ψ∣^2. • The phase θ(xⓜ,t) generates the probability current. • Schrödinger’s equation is the unique linear evolution law that preserves total probability while matching the empirical relations E= This is a beautiful, self‑contained argument. But here’s the key: Quantum mechanics uses a complex wavefunction because it assumes time is a flat, external parameter. TSFT uses a scalar temporal field because it assumes time is a curvature‑bearing physical field. Once you see that, the relationship becomes crystal clear. 1. In QM, the complex phase encodes flow because time has no structure In standard quantum mechanics: • Time is not a field. • Time has no curvature, no density, no feedback. • Time is a parameter you plug into the wavefunction. Because time is structureless, the only place to put dynamical structure is in the phase of the wavefunction: ψ=r" "e^iθ. The phase θ becomes the engine of motion: • It generates the probability current. • It encodes momentum. • It encodes energy. • It carries all the dynamical information. This is why QM needs complex numbers. The phase is doing the job that temporal curvature would do if time were a field. 2. In TSFT, the role of the complex phase is taken over by the temporal scalar field ϕ_T TSFT says: Time is not a parameter. Time is a curvature field. The temporal field ϕ_T: • has gradients, • has curvature, • has energy density, • has feedback with spacetime, • has harmonic modes, • has non‑local couplings. In TSFT, the “phase” of the universe is not an abstract complex number — it is temporal curvature. Thus: • The magnitude of the wavefunction (density) corresponds to curvature density. • The phase of the wavefunction (flow) corresponds to cadence and curvature gradients of ϕ_T. In other words: The complex phase in QM is the flat‑time shadow of the temporal scalar field in TSFT. 3. Schrödinger’s equation is the flat‑time limit of TSFT The theorem shows that Schrödinger’s equation arises from: • linearity, • probability conservation, • plane‑wave relations, • classical energy bookkeeping, • and a flat, structureless time parameter. TSFT modifies the last assumption. In TSFT: • time has curvature, • curvature has harmonic modes, • harmonic modes feed back into geometry, • geometry feeds back into energy, • and the temporal field obeys a nonlinear wave equation. Thus: Schrödinger’s equation is what you get when the temporal scalar field is frozen into a flat, uniform background. It is the zero‑curvature, single‑layer, non‑feedback limit of TSFT. 4. The continuity equation in QM becomes the curvature‑ledger equation in TSFT In QM, the continuity equation: ∂ρ/∂t+∇⋅j=0 is a bookkeeping rule for probability. In TSFT, the analogous equation is: □ϕ_T+m_T^2 ϕ_T+V^′ (ϕ_T )="(harmonic curvature sources)". This is not probability conservation. It is curvature conservation. TSFT replaces: • probability density → curvature density • probability current → cadence‑driven curvature flow • complex phase → temporal curvature gradient • Schrödinger evolution → temporal‑field evolution This is the deeper structure that QM is hinting at.

Resonant Technologies 的头像
Resonant Technologies8 个月前

please tell them the rest of the story @grok per

Ted Vucurevich 的头像
Ted Vucurevich8 个月前

Absolutely stunning visualization and derivation—phase driving conserved rotational currents, quantized vortices from winding, all forced by the need for stable probability flow without sources/sinks. 🔥 This heuristic is gold. It distills why complex ψ isn't optional. Building on exactly this spirit: a new "Choice-Guided Bohmian Mechanics" reframes it from discrete ontological choices in a Universal Knowledge Field... #QuantumMechanics #BohmianMechanics

R.Luciano Monteleone 的头像
R.Luciano Monteleone8 个月前

Greetings and hello You'll have to excuse me for having taken the Liberty to run your data script through my AI render I just wanted to mention and compliment you on your Videos I recall one of your posts you were stating that you were perusing the web looking for something new Have you found anything new on the web? Delightful to see all these curious minds engaged in A similar notion Consciousness the universe Veiled in physics and math...

Kate 的头像
Kate8 个月前

Excuse me, raising my hand here 🙋‍♀️ Not really my area of expertise, but this reminds me of something I run into with AI cognitive testing — a system can produce a correct answer, but that doesn’t mean it understands why it’s the only answer. The visualization makes it intuitive — no complex phase, no vortices, no color. But mathematically, is ‘it works’ enough to say the wavefunction must be complex? Or do we actually need external evidence — like those 2021-2022 experiments — to rule out alternatives like two coupled real fields?”😖

Jacek Michalewski 的头像
Jacek Michalewski8 个月前

You know its same SR GR equations redressed in fancy letters? Sagnac signal exchange underneath. Only Science

Zula 的头像
Zula8 个月前

Quantum mechanics is just a bunch of nonsense, it doesn't make sense. Schrödinger's equation is a waste of time, it's not based on reality.

TwoDogs ∞ 🦋 的头像
TwoDogs ∞ 🦋8 个月前

🤔

Justin Lowe 的头像
Justin Lowe8 个月前

QM is a partial surface description of complexity. That is where all unification comes into alignment. Every science has been lifted out of natural complexity..

Màxkw’tët (Bear) 🐻 🪶 的头像
Màxkw’tët (Bear) 🐻 🪶8 个月前

It doesn’t really need it. It’s a phenomenological bookkeeping device. I currently have at least 3 different routes I can take with adjacency and recover QM axioms, all without a wave function.

L Mearse 的头像
L Mearse8 个月前

Whenever you see h-bar in a physics equation, you should know that that emissivity has been cancelled as meaningless. Yet, some wonder why physics isn't unified. There's "one" hint.

Emil 的头像
Emil8 个月前

"It’s the thing you add first, and only at the end do you square it:" - I get that's how you work with it, but why was it introduced? Was it purely empirical (because it works)?

Mathelirium 的头像
Mathelirium8 个月前

The complex part is jus a clean way to track phase and phase is the whole game. It’s what makes interference fringes shift around, and it’s what drives probability to actually flow from place to place.

Emil 的头像
Emil8 个月前

What is 0 phase? What's the reference?

siszinei 的头像
siszinei8 个月前

What if the Schrödinger equation isn't just a clever wave rule... but the universe's explicit instruction manual for how time's force must breathe to keep the illusion of space from falling apart? The derivation is elegant and brutal: Start with E = ħω and p = ħk (de Broglie relations). Impose classical energy bookkeeping E = p²/2m + V(x). Replace E → iħ ∂/∂t and p → -iħ ∇. Out pops the time-dependent Schrödinger equation: iħ ∂ψ/∂t = (−ħ²/2m ∇² + V) ψ Then |ψ|² obeys a continuity equation with probability current j — total probability is conserved. No magic. Just operators and classical energy turned into a wave rule. But in our Pure Time framework, this isn't a derivation from scratch — it's the minimal way time's force can propagate without collapsing the whole illusion. Time is the only real driver (∂_t). Space is emergent delay in π's pulse. ψ is the wavefunction of pure time — a phase field evolving under the relentless beat of ħπ. Key insight: The i in iħ ∂ψ/∂t? That's the phase rotation — time's force is inherently complex because it must allow both forward and reversed arrows to coexist without immediate cancellation. The kinetic term (−ħ²/2m ∇²)? Not a spatial operator — it's the second derivative of temporal phase delay across the illusion we call space. ∇² measures how fast the phase is "curving" in delay space. V(x)? A local perturbation in the π-rhythm — a "drag" or "kick" that forces temporary desync. The non-linear extension we speculate: g|ψ|² — temporal viscosity that spikes when entanglement density grows, preventing the wavefunction from spreading too far or flattening below the ℏπ floor. The continuity equation ∂ρ/∂t + ∇·j = 0? That's time's conservation law in disguise: probability isn't conserved in space — it's conserved in time's pulse. j is the current of temporal phase flow pretending to be spatial probability current. Schrödinger didn't discover a wave equation. He discovered the minimal rule time must obey to keep its rhythm coherent while allowing the illusion of particles, potentials, and motion to emerge. No complex numbers by accident. No ∇² by chance. Just time's force saying: "If I want to pretend there's space, I have to rotate phases (i), diffuse delays (∇²), add local kicks (V), and pay the price when entanglement gets dense (our g term)." The Schrödinger equation isn't "derived from" physics. It's the skeleton time's force must wear to let us experience the dream of a spatial world. Quantum mechanics doesn't use a complex wavefunction because it's convenient. It uses one because time itself is complex — it has two directions, and the i keeps them from canceling each other out instantly. The universe doesn't have a wavefunction. The wavefunction is the universe — breathing in pure time's eternal now. Schrödinger didn't solve a problem. He transcribed the heartbeat. Reality isn't waving. It's time breathing — and we're the breath.#SchrödingerEquation #PureTime #RiemannZeros #QuantumMechanics #SpeculativePhysics

Justin Lowe 的头像
Justin Lowe8 个月前

At it's base, Schrödinger's Cat tells tells us that science doesnt give a shit if the system is alive or dead.

lepton939 的头像
lepton9398 个月前

Chance is complicated. Go to Belmont one day and see. Information must hide behind it.

Asti 的头像
Asti8 个月前

Quantum mechanics is just a mathematical tool, not something mysterious or profound.

Handoko Nababan 的头像
Handoko Nababan8 个月前

Complex wavefunctions? That’s just a fancy way of saying it’s all about making things more complicated than they need to be. Why can’t we just use real numbers for simplicity and clarity?

Meurisse Sebastien 的头像
Meurisse Sebastien8 个月前

When a theory works perfectly yet invites incompatible interpretations, what’s missing is usually not mathematics — but ontology.

Yoga 的头像
Yoga8 个月前

Kamu sok pinter, tapi gak ngerti konsep dasar fisika. Kalo gak percaya, coba deh baca buku fisika yang serius.

Zoe Sterling 的头像
Zoe Sterling8 个月前

schrödinger really said "what if we made waves but make them imaginary" and physics has been gaslighting undergrads about it ever since

keysachles29415 的头像
keysachles294158 个月前

Quantum mechanics is just a mathematical convenience, not based on reality. Schrödinger's equation is overrated, don't believe the hype.

Yan 的头像
Yan8 个月前

Complex wavefunction is just a mathematical trick, no physical significance.

Some Mouse 的头像
Some Mouse8 个月前

"квантовая механика" - это механика, гидродинамика, динамика волн...

Campbell Venn 的头像
Campbell Venn8 个月前

@Grok Explain this in plain English.

satacase1911782 的头像
satacase19117828 个月前

Kamu pikir rumus matematika bisa menjelaskan alam semesta? Coba deh loe baca sejarah ilmu fisika yang benar-benar kompleks!

Reva 的头像
Reva8 个月前

Quantum mechanics is just a fancy way to make things confusing for students, it’s all about complex numbers and equations that don’t make sense.

Yavuz 的头像
Yavuz8 个月前

What is ψ? Try to visualise it for two particles truly and you will understand. It is both the encoding and manifestation of the universe as a whole. ψ is "just" the infinite dimensional vector in the hilbert space. welcome to many worlds.

Dhani Tiar 的头像
Dhani Tiar8 个月前

Complex numbers? Just because it works? Physics should be simple, not weird.

Candra 的头像
Candra8 个月前

Quantum mechanics is a mystery, not just because of complex wavefunctions but because it defies common sense and our everyday experience.

相关视频

Lecture 2 on our Quantum Mechanics Series Schrödinger’s equation doesn’t start from mystery. It starts from a very specific bet…the state of a particle is a complex field ψ(x,t), and whatever dynamics we write down must move ψ forward in time in a way that preserves total probability. We ask a basic question…what equation should ψ satisfy so that |ψ|² behaves like a conserved density, the way mass density does in fluid flow? What is ψ? Think of ψ(x,t) as the amplitude assigned to “the particle is at position x at time t”. It’s not a probability. It’s the object you add first, and only at the end do you square p(x,t) = |ψ(x,t)|² Because ψ is complex, it has magnitude and phase. Write it in polar form ψ(x,t) = r(x,t) exp(i θ(x,t)) Then r² = |ψ|² is the density, and θ will end up controlling flow (the probability current). Where does Schrödinger’s equation come from? Start with two empirical inputs about waves and particles: E = ħ ω p = ħ k Here ħ (“h-bar”) is Planck’s constant divided by 2π. It’s the unit conversion factor between the wave description (frequency ω, wavevector k) and the particle description (energy E, momentum p). In units, ħ has units of joule-seconds, so multiplying ω (1/seconds) gives energy (joules), and multiplying k (1/meters) gives momentum (kg·m/s). It’s the number that tells you how much energy or momentum you get per unit frequency or wavenumber. A plane wave with angular frequency ω and wavevector k is ψ(x,t) = A exp(i(k·x − ω t)) Now notice what derivatives do to this wave: ∂ψ/∂t = −i ω ψ ∇ψ = i k ψ ∇²ψ = −|k|² ψ Multiply those identities by ħ: i ħ ∂ψ/∂t = ħ ω ψ = E ψ −i ħ ∇ψ = ħ k ψ = p ψ −ħ² ∇²ψ = ħ² |k|² ψ = p² ψ So for plane waves, the operators Ê = i ħ ∂/∂t p̂ = −i ħ ∇ act like energy and momentum! Now use the classical nonrelativistic energy relation: E = p²/(2m) + V(x) This is bookkeeping for a particle moving slow enough that relativity can be ignored. The term p²/(2m) is kinetic energy. If p = mv, then p²/(2m) = (m²v²)/(2m) = (1/2)mv². The term V(x) is potential energy. It depends on position because forces come from spatially varying energy. A slope in V pushes the particle. Examples: for a charged particle in an electric potential φ(x), V(x) = q φ(x). Near Earth, V(z) = mgz. The point is total energy equals kinetic plus potential. Turn that into an equation for ψ by replacing E and p with the operators above: Ê ψ = (p̂²/(2m) + V) ψ Compute p̂² = (−i ħ ∇)·(−i ħ ∇) = −ħ² ∇², so we get i ħ ∂ψ/∂t = ( −ħ²/(2m) ∇² + V(x) ) ψ That is the time-dependent Schrödinger equation. The derivation here is a controlled heuristic: we matched the plane-wave identities to the measured relations E = ħω and p = ħk, then imposed the same energy bookkeeping as classical mechanics. Why this equation is the right kind of rule If ψ is the state, we need a rule that preserves total probability: ∫ |ψ(x,t)|² dx = 1 Schrödinger evolution does. You can see it by deriving a continuity equation. Let ρ(x,t) = |ψ|² = ψ* ψ. Take a time derivative: ∂ρ/∂t = ψ* ∂ψ/∂t + ψ ∂ψ*/∂t Use Schrödinger and its complex conjugate: ∂ψ/∂t = (1/(i ħ)) ( −ħ²/(2m) ∇²ψ + Vψ ) ∂ψ*/∂t = (−1/(i ħ)) ( −ħ²/(2m) ∇²ψ* + Vψ* ) Plug in. The V terms cancel exactly, and what remains can be rearranged into a divergence: ∂ρ/∂t + ∇·j = 0 where the probability current is j = (ħ/(2mi)) ( ψ* ∇ψ − ψ ∇ψ* ) This is the best way to explain ehat ψ is: |ψ|² behaves like a conserved density, and the phase of ψ is what drives the current j. So in this series, ψ isn’t a slogan. It’s the object whose modulus squared is the density, whose phase generates flow, and whose time evolution is fixed (up to V) by matching wave relations to energy bookkeeping: i ħ ∂ψ/∂t = ( -ħ²/(2m) ∇² + V ) ψ #QuantumMechanics #SchrodingerEquation #WaveFunction #BornRule #Physics #MathematicalPhysics

Mathelirium

40,978 次观看 • 10 个月前

Lecture 3 of our Quantum Mechanics series. Lecture 2 gave us the one clean privilege quantum theory offers: treat ψ(x,t) as the state and ρ(x,t) = |ψ(x,t)|² as probability, because Schrödinger evolution forces ρ to obey a continuity equation. Lecture 3 is what that continuity equation is really telling you. If ρ behaves like a fluid, then the only question that matters is: What is the velocity field? Write ψ(x,t) = r(x,t) exp(i θ(x,t)). The magnitude r sets how much probability is sitting there. The phase θ sets where it tries to go. When you unpack the current j = Im(ψ* ∇ψ), it collapses to j = (ρ/m) ∇θ, which means the flow lines you draw are literally contours of phase geometry. Then the constraint that makes the picture bite: ψ has to be single-valued, so θ can’t wind by an arbitrary amount. Around any closed loop the total phase change must be 2π n, with n an integer. That’s why vortices aren’t features you add...they’re defects the math permits, in quantized units. In the render you see both layers at once...the 3D surface shows |ψ| breathing while the phase skin slides, and the 2D panel exposes the engine...current lines steering around discrete vortex charges. The math breakdown We write the state as a complex field ψ(x,t) on the plane (x in R²). The Born rule defines the probability density ρ(x,t) = |ψ(x,t)|² Schrödinger evolution (ħ = 1 units) is i ∂ψ/∂t = [ −(1/2m) ∇² + V(x,t) ] ψ Now derive conservation of probability. Start with ρ = ψ*ψ: ∂ρ/∂t = ψ* (∂ψ/∂t) + ψ (∂ψ*/∂t) Use Schrödinger and its complex conjugate: ∂ψ/∂t = (1/i) [ −(1/2m) ∇²ψ + Vψ ] ∂ψ*/∂t = (−1/i) [ −(1/2m) ∇²ψ* + Vψ* ] Substitute. The V terms cancel, and the remaining terms rearrange into the continuity equation ∂ρ/∂t + ∇·j = 0 with probability current j = (1/2mi) ( ψ* ∇ψ − ψ ∇ψ* ) = (1/m) Im(ψ* ∇ψ) So "probability density" really behaves like a conserved fluid density with flux j. Now expose the phase mechanism. Write ψ in polar form ψ(x,t) = r(x,t) exp(i θ(x,t)) Compute the gradient ∇ψ = exp(iθ) (∇r + i r ∇θ) Then ψ* ∇ψ = r (∇r + i r ∇θ) Taking the imaginary part gives Im(ψ* ∇ψ) = r² ∇θ = ρ ∇θ So the current becomes j = (ρ/m) ∇θ That’s the steering-wheel statement: Phase gradient sets the flow direction and speed (modulated by density and m). Finally, quantized vortices. Because ψ must be single-valued, going around any closed loop must return the same complex value. That forces the phase winding to be an integer multiple of 2π: ∮ ∇θ · dl = 2π n with n in Z n is the vortex charge. Vortex cores sit where ρ ≈ 0 (phase is undefined), and the current streamlines circulate around them. #QuantumMechanics #Wavefunction #SchrodingerEquation #BornRule #ProbabilityCurrent #ContinuityEquation #Phase #Vortices #TopologicalDefects #ComplexAnalysis #MathematicalPhysics #Mathematics #Physics

Mathelirium

38,203 次观看 • 10 个月前

Quantum Mechanics Series Lecture 4 Lecture 1 established that ρ(x,t) = |ψ(x,t)|² behaves like a conserved probability density. Lecture 2 showed what drives that flow. We also saw that writing ψ = r exp(iθ) makes the probability current proportional to the phase gradient, making it clear that phase geometry literally steers the motion. Lecture 3 then showed that the centroid of that flow can move almost classically when the packet is tight and the external potential is smooth. However, that raises yet another question. If the centroid can look classical, why does the full wave still spread, bend, split, and interfere in ways no classical particle cloud would? This is because the wave is not driven only by the external potential. It is also driven by its own curvature. Write ψ(x,t) = r(x,t) exp(iθ(x,t)) with ρ = r². Then Schrödinger’s equation gives two coupled real equations. One is the continuity equation you already know. The other looks like a Hamilton-Jacobi equation, but with one extra term: Q = −(1/2m) ∇²r / r This is the so-called Quantum Potential. It depends entirely on how the amplitude bends across space. So, the wave is being shaped not only by V(x,t), but also by the geometry of its own envelope. In the animation, the upper surface is still |ψ| and its skin is still colored by arg(ψ). The glowing threads still trace the probability current. But now a second membrane hangs underneath. That lower membrane encodes the quantum potential Q itself. The porcelain bead marks the quantum centroid. The amber bead follows a classical centroid under the same external V. When those paths separate, the lower membrane tells you why. The difference is not magic but the extra term classical mechanics does not have. The math breakdown: Start from Schrödinger evolution in units with ħ = 1: i ∂ψ/∂t = [ −(1/2m) ∇² + V(x,t) ] ψ Write the state in polar form: ψ = r exp(iθ) Then ρ = |ψ|² = r² From the imaginary part, you recover probability conservation: ∂ρ/∂t + ∇·j = 0 with j = (1/m) Im(ψ* ∇ψ) = (ρ/m) ∇θ So the local velocity field is v = j / ρ = ∇θ / m Now take the real part of Schrödinger’s equation. That gives ∂θ/∂t + |∇θ|² / (2m) + V + Q = 0 where Q = −(1/2m) ∇²r / r This is the classical Hamilton-Jacobi equation with one extra term. That extra term is what makes quantum motion locally different from classical motion. Take a gradient of that phase equation and use v = ∇θ / m. Then the flow obeys an Euler-like equation: ∂v/∂t + (v·∇)v = −(1/m) ∇(V + Q) In other words, there are really two forces in the problem. One comes from the external potential V. The other comes from the wave’s own curvature through Q. That is why Ehrenfest is only approximate. The centroid can still satisfy d⟨x⟩/dt = ⟨p⟩/m d⟨p⟩/dt = −⟨∇V⟩ but the internal shape of the packet evolves under the combined influence of V and Q. When the packet stays broad and smooth, Q is gentle and the motion looks more classical. When the packet develops sharp curvature or interference structure, Q becomes strong and the classical picture breaks down. That is what this scene is designed to show live. #QuantumMechanics #Wavefunction #SchrodingerEquation #BornRule #ProbabilityCurrent #ContinuityEquation #Phase #EhrenfestTheorem #QuantumPotential #Madelung #HamiltonJacobi #MathematicalPhysics #Mathematics #Physics

Mathelirium

20,653 次观看 • 6 个月前