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A magnetic field reshapes a Potassium atom's Rydberg electron cloud into a rotating quantum flower.

Mathelirium

80,238 subscribers

10,263 görüntüleme • 11 gün önce •via X (Twitter)

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Henning Sittler profil fotoğrafı

Henning Sittler11 gün önce

Mathelerium animated periodic table?

Mathelirium profil fotoğrafı

Mathelirium11 gün önce

Yes😄

AYM profil fotoğrafı

AYM11 gün önce

how she makes me feel

turn profil fotoğrafı

turn10 gün önce

It looks to me like two top to tip tits and nipples. Did I get my “math” mixed up with “tetesterone”? smh

Ax profil fotoğrafı

Ax11 gün önce

Wow wow wow

mukh profil fotoğrafı

mukh11 gün önce

looks familiar

SPORTS EVANGELIST IS NOT SPORTS ILLUSTRATED profil fotoğrafı

SPORTS EVANGELIST IS NOT SPORTS ILLUSTRATED11 gün önce

@grok please

Mitleidstour profil fotoğrafı

Mitleidstour11 gün önce

Viel Spaß 😬

Frank Clarke profil fotoğrafı

Frank Clarke11 gün önce

It's thermal dynamic presure that forms anything to the memery of watter at 00resonance resonance and Fibonacci is it's bace line Vera Rubin, Nikola Tesla, Albert Einstein, Gérard Gremaud, Konstantin Meyl, Ferenc Takács — these understand G13 but have not seen((Q(Hi? %%%hn.

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This is a Rubidium Rydberg wavepacket reshaped by an external electric field. The electron is not shown as a particle. The surface represents regions of high probability density, |Ψ|², while the colours show the quantum phase, arg(Ψ).

This is a Rubidium Rydberg wavepacket reshaped by an external electric field. The electron is not shown as a particle. The surface represents regions of high probability density, |Ψ|², while the colours show the quantum phase, arg(Ψ).

Mathelirium

12,944 görüntüleme • 12 gün önce

This is a visualization of a Rydberg wavepacket. In simple terms it is a way of showing an electron in a very highly excited quantum state. The Math comes from the Schrödinger equation for hydrogen where the electron is described by a wavefunction rather than as a tiny ball moving on a fixed path. The yellow sphere at the centre is the proton, not the electron. The colored 3D surface around it shows places where the electron is more likely to be, i.e. a probability cloud.

This is a visualization of a Rydberg wavepacket. In simple terms it is a way of showing an electron in a very highly excited quantum state. The Math comes from the Schrödinger equation for hydrogen where the electron is described by a wavefunction rather than as a tiny ball moving on a fixed path. The yellow sphere at the centre is the proton, not the electron. The colored 3D surface around it shows places where the electron is more likely to be, i.e. a probability cloud.

Mathelirium

17,580 görüntüleme • 1 ay önce

Now, we move on to Sodium, where the quantum geometry becomes even richer. Here, the valence electron is built from a coherent superposition of s, p, and d Rydberg states. Because these three families experience the Sodium core differently, their energies are shifted by different quantum defects. Their phases therefore drift apart and reunite at different rates.

Now, we move on to Sodium, where the quantum geometry becomes even richer. Here, the valence electron is built from a coherent superposition of s, p, and d Rydberg states. Because these three families experience the Sodium core differently, their energies are shifted by different quantum defects. Their phases therefore drift apart and reunite at different rates.

Mathelirium

27,698 görüntüleme • 15 gün önce

The positron is the antimatter partner of the electron and together they form positronium... a tiny quantum system with no nucleus. We used the time-dependent Schrödinger equation to evolve the electron and positron clouds. Their motion comes from their quantum states changing over time and the color from phase.

The positron is the antimatter partner of the electron and together they form positronium... a tiny quantum system with no nucleus. We used the time-dependent Schrödinger equation to evolve the electron and positron clouds. Their motion comes from their quantum states changing over time and the color from phase.

Mathelirium

26,253 görüntüleme • 8 gün önce

$A relativistic electron beam can radiate without striking the metal at all. As the microbunches skim the periodic grating, their evanescent EM field is diffracted into radiation, producing angled wavefronts$

A relativistic electron beam can radiate without striking the metal at all. As the microbunches skim the periodic grating, their evanescent EM field is diffracted into radiation, producing angled wavefronts

Mathelirium

14,810 görüntüleme • 24 gün önce

This is a computational electromagnetics simulation of a magnetron. A magnetron is a high-power microwave oscillator that uses crossed electric and magnetic fields to control electrons inside resonant cavities. Here, electrons emitted from the central cathode begin to organize into rotating spokes. As they phase-lock with the cavity field, they transfer energy into the resonant microwave mode and sustain the oscillation. Magnetrons are used in microwave ovens, radar systems, industrial heating, plasma generation, and high-power microwave sources.

This is a computational electromagnetics simulation of a magnetron. A magnetron is a high-power microwave oscillator that uses crossed electric and magnetic fields to control electrons inside resonant cavities. Here, electrons emitted from the central cathode begin to organize into rotating spokes. As they phase-lock with the cavity field, they transfer energy into the resonant microwave mode and sustain the oscillation. Magnetrons are used in microwave ovens, radar systems, industrial heating, plasma generation, and high-power microwave sources.

Mathelirium

12,992 görüntüleme • 17 gün önce

A Quantum Current Chooses a Path A single electron enters a microscopic interferometer, but its wavefunction travels through two routes at once. One branch crosses a resonant quantum dot while the other moves freely around a ring threaded by magnetic flux. The probability current is j = (ℏ/m) Im(ψ*∇ψ) - (q/m)A|ψ|², while the enclosed flux creates the Aharonov-Bohm phase Δφᴬᴮ = qΦ/ℏ. The quantum dot adds the resonant phase δ(E) = atan2(Γ, E - E₀), producing Fano interference when the two paths recombine. Wave packets split, become temporarily trapped, form circulating current vortices, reverse direction after a flux quench, and finally escape through the drain in a coherent burst. The glowing threads are material curves transported by v = j/ρ, revealing how invisible quantum phase controls the flow. #QuantumMechanics #AharonovBohmEffect #QuantumInterference #QuantumDot #ProbabilityCurrent #MesoscopicPhysics #PhysicsAnimation #Physics

A Quantum Current Chooses a Path A single electron enters a microscopic interferometer, but its wavefunction travels through two routes at once. One branch crosses a resonant quantum dot while the other moves freely around a ring threaded by magnetic flux. The probability current is j = (ℏ/m) Im(ψ*∇ψ) - (q/m)A|ψ|², while the enclosed flux creates the Aharonov-Bohm phase Δφᴬᴮ = qΦ/ℏ. The quantum dot adds the resonant phase δ(E) = atan2(Γ, E - E₀), producing Fano interference when the two paths recombine. Wave packets split, become temporarily trapped, form circulating current vortices, reverse direction after a flux quench, and finally escape through the drain in a coherent burst. The glowing threads are material curves transported by v = j/ρ, revealing how invisible quantum phase controls the flow. #QuantumMechanics #AharonovBohmEffect #QuantumInterference #QuantumDot #ProbabilityCurrent #MesoscopicPhysics #PhysicsAnimation #Physics

Mathelirium

16,684 görüntüleme • 2 ay önce

A single electron can make a pair of metallic nanostructures glow. As it passes through a metallic bowtie gap, its near field excites surface plasmons, concentrating energy into a tiny hotspot before releasing it as light. This is known as Cathodoluminiscence. It is a process of revealing hidden optical modes at the nanoscale.

A single electron can make a pair of metallic nanostructures glow. As it passes through a metallic bowtie gap, its near field excites surface plasmons, concentrating energy into a tiny hotspot before releasing it as light. This is known as Cathodoluminiscence. It is a process of revealing hidden optical modes at the nanoscale.

Mathelirium

15,174 görüntüleme • 1 ay önce

A Schrödinger quantum wave packet moves into a double barrier, swells inside the resonant chamber, and then tunnels through.

A Schrödinger quantum wave packet moves into a double barrier, swells inside the resonant chamber, and then tunnels through.

Mathelirium

29,608 görüntüleme • 5 ay önce

Magnetism can behave like a spectrum like light. In the Searl Effect, a rotating magnetic field forms a sine-wave pattern where energy flows along the wave. Like a river: the oscillating magnetic field becomes the channel that guides moving charge and energy downstream.

Magnetism can behave like a spectrum like light. In the Searl Effect, a rotating magnetic field forms a sine-wave pattern where energy flows along the wave. Like a river: the oscillating magnetic field becomes the channel that guides moving charge and energy downstream.

Bluntly Put Philosopher (BPP)

16,731 görüntüleme • 6 ay önce

A Bonus render of Electron Holography for our Quantum Mechanics Lecture Series. We’re staging a TEM-style electron holography shot as a single 3D scene. A coherent electron wave ψ(x,y,t) enters from the left as a localized packet, gets split by a thin biprism phase wedge, then bends around a central nanoring that stands in for an enclosed magnetic flux. The wave evolves by Schrödinger dynamics, so its intensity ρ=|ψ|² is literally the electron detection probability density, while the probability current j=(1/m)Im(ψ*∇ψ) acts like a conserved flow of that density across the plane. The main surface is a living whose height tracks |ψ| and whose skin color cycles with arg(ψ). On top of it, luminous current ribbons trace streamlines of v=j/(ρ+ε), so you can see how phase gradients steer the flow around the ring and back into interference. High above, a tilted detector/hologram screen shows the off-axis fringe image you’d measure (intensity after mixing with a reference wave), while a porcelain bead marks the centroid ⟨x⟩(t) and flux threads through the ring pulse in sync with the Aharonov-Bohm phase knob φ_AB(t). See our lecture series for details. #QuantumMechanics #ElectronHolography #MathematicalPhysics #Physics

A Bonus render of Electron Holography for our Quantum Mechanics Lecture Series. We’re staging a TEM-style electron holography shot as a single 3D scene. A coherent electron wave ψ(x,y,t) enters from the left as a localized packet, gets split by a thin biprism phase wedge, then bends around a central nanoring that stands in for an enclosed magnetic flux. The wave evolves by Schrödinger dynamics, so its intensity ρ=|ψ|² is literally the electron detection probability density, while the probability current j=(1/m)Im(ψ*∇ψ) acts like a conserved flow of that density across the plane. The main surface is a living whose height tracks |ψ| and whose skin color cycles with arg(ψ). On top of it, luminous current ribbons trace streamlines of v=j/(ρ+ε), so you can see how phase gradients steer the flow around the ring and back into interference. High above, a tilted detector/hologram screen shows the off-axis fringe image you’d measure (intensity after mixing with a reference wave), while a porcelain bead marks the centroid ⟨x⟩(t) and flux threads through the ring pulse in sync with the Aharonov-Bohm phase knob φ_AB(t). See our lecture series for details. #QuantumMechanics #ElectronHolography #MathematicalPhysics #Physics

Mathelirium

14,252 görüntüleme • 8 ay önce

A Schrödinger quantum wave packet moves into a double barrier, swells inside the resonant chamber, and then tunnels through.

A Schrödinger quantum wave packet moves into a double barrier, swells inside the resonant chamber, and then tunnels through.

Mathelirium

25,597 görüntüleme • 4 ay önce

An Electron flies above a metal grating without touching it. As the electron passes, each groove scatters its electromagnetic near field at a slightly different time. The emissions interfere and produce what's called Smith-Purcell radiation. This effect is being explored for tunable Terahertz radiation, biomedical spectroscopy, and high-speed communications.

An Electron flies above a metal grating without touching it. As the electron passes, each groove scatters its electromagnetic near field at a slightly different time. The emissions interfere and produce what's called Smith-Purcell radiation. This effect is being explored for tunable Terahertz radiation, biomedical spectroscopy, and high-speed communications.

Mathelirium

21,005 görüntüleme • 1 ay önce

TEACHING LESSON: Here you can see the effect of a 3-phase, rotating magnetic field on a permanent ball-shaped magnet. Spin, baby, spin! 🛸

TEACHING LESSON: Here you can see the effect of a 3-phase, rotating magnetic field on a permanent ball-shaped magnet. Spin, baby, spin! 🛸

Red Collie (Dr. Horace Drew) scientist/inventor

29,869 görüntüleme • 1 yıl önce

A sub-wavelength slit in a dispersive metal turns an incoming electromagnetic pulse into a strongly structured transmitted field.

A sub-wavelength slit in a dispersive metal turns an incoming electromagnetic pulse into a strongly structured transmitted field.

Mathelirium

47,063 görüntüleme • 24 gün önce

When gravitational potential rotates, it can lock onto an orbit’s phase and start rearranging motion. Order can turn into visible structure, and structure can slide into chaos, without any collisions or extra bodies. This is a toy barred galaxy...a softened central potential plus a rotating bar-shaped overdensity. The bar's angle sways and wobbles, and its strength breathes over time, so the force field keeps changing.

When gravitational potential rotates, it can lock onto an orbit’s phase and start rearranging motion. Order can turn into visible structure, and structure can slide into chaos, without any collisions or extra bodies. This is a toy barred galaxy...a softened central potential plus a rotating bar-shaped overdensity. The bar's angle sways and wobbles, and its strength breathes over time, so the force field keeps changing.

Mathelirium

10,118 görüntüleme • 7 ay önce

Erwin Schrödinger’s 1926 equation turned quantum mechanics into wave dynamics. Instead of tracking a particle by a sharp trajectory, you evolve a complex wavefunction whose shape and phase carry the physics.

Erwin Schrödinger’s 1926 equation turned quantum mechanics into wave dynamics. Instead of tracking a particle by a sharp trajectory, you evolve a complex wavefunction whose shape and phase carry the physics.

Mathelirium

168,325 görüntüleme • 6 ay önce

A rapidly rotating magnetic field creates a stable “bound state,” letting repelling magnets orbit without touching. It’s a striking example of how dynamic fields can produce unexpected stability. Sudanamaru (Hamdi Ucar)

A rapidly rotating magnetic field creates a stable “bound state,” letting repelling magnets orbit without touching. It’s a striking example of how dynamic fields can produce unexpected stability. Sudanamaru (Hamdi Ucar)

Bluntly Put Philosopher (BPP)

296,809 görüntüleme • 1 ay önce

Copper itself is not magnetic. However, the magnetic field causes electrons on the surface of the copper to rearrange themselves and begin rotating. This is the interaction of a magnet and copper. [📹styro.drake]

Copper itself is not magnetic. However, the magnetic field causes electrons on the surface of the copper to rearrange themselves and begin rotating. This is the interaction of a magnet and copper. [📹styro.drake]

Massimo

140,499 görüntüleme • 26 gün önce