5 items · 2 systems

2026-09-25 Fri

Science & Physics

3

  1. 01

    A Bayesian ringdown analysis of GW250114 makes the first direct measurement of the 220x220 quadratic quasi-normal-mode amplitude-coupling coefficient, finding it consistent with numerical-relativity and second-order-perturbation-theory predictions to within 1.3 sigma in every comparison

    [2026-09-25] · src Yang, Shi, Hu; arXiv:2609.28953 (2026-09-24)

    • gravitational waves
    • black hole ringdown
    • general relativity tests

    Second-order black-hole perturbation theory predicts that a ringdown's quadratic (nonlinear) quasi-normal modes should have amplitudes scaling as the product of their parent linear modes' amplitudes, with a coupling coefficient that depends on the remnant's spin - but that coefficient had never been directly measured from real gravitational-wave data. Yang, Shi and Hu model the GW250114 ringdown with the 220, 221 and 220x220 modes and use Bayesian inference to extract the amplitude-coupling coefficient of the 220x220 mode. The inferred value is consistent with both numerical-relativity fits and second-order perturbation theory, with no comparison showing a deviation exceeding 1.3 sigma - though the data are not yet precise enough to pick between the spin-dependent variants of the prediction.

    Why

    This is a calibrated non-result in the best sense: nonlinear black-hole dynamics, previously verified only in numerical-relativity simulations, now has a real measurement to compare against, and general relativity passed the first check available to it. The paper is explicit that current sensitivity cannot yet distinguish between competing spin-dependent predictions for the coupling coefficient, so what this establishes is the method rather than a tight constraint - the next loud ringdown, or a longer stack of them, is what turns "consistent with GR" into a genuine test able to rule something out.

  2. 02

    A cryogenic planar metallo-dielectric antenna coupled to a single dibenzoterrylene molecule delivers 100 million collected photons per second at 97% collection efficiency, with 91.2% two-photon indistinguishability on the Fourier-limited transition and 97.7% single-photon purity under both continuous-wave and pulsed excitation

    [2026-09-25] · src Luo, Hebenstreit, Shkarin, Renger, Utikal, Goetzinger; arXiv:2609.29736 (2026-09-24)

    • quantum photonics
    • single photon sources
    • organic molecules

    Single-photon sources for quantum networking and metrology need brightness, indistinguishability and purity simultaneously, and organic dye molecules - which emit transform-limited photons at cryogenic temperature without the growth complexity of a quantum dot - have historically lost on brightness because so little of their emission was ever collected. Luo et al. couple a single dibenzoterrylene molecule to a cryogenic planar metallo-dielectric antenna designed to funnel its emission toward collection optics, reaching a 97% collection efficiency and a detected rate of 100 million photons per second, while the photons themselves show 91.2% indistinguishability on the molecule's Fourier-limited transition and 97.7% single-photon purity under both continuous-wave and pulsed excitation.

    Why

    No single number here is unprecedented on its own, but having all three - rate, indistinguishability and purity - at once from a chemically simple emitter is what the paper is actually claiming: organic molecules move from a laboratory curiosity to a platform competitive with the quantum-dot and defect-center sources that have dominated photonic quantum information work. What that buys downstream is a simpler, more reproducible fabrication route to a component - the deterministic single-photon source - that photonic quantum computing and quantum-repeater schemes both depend on and have long found hard to source at scale.

  3. 03

    Twisted Bernal bilayer-trilayer graphene hosts tunable Chern insulators up to |C|=3 across twist angles 1.05-1.50 degrees, and at theta=1.18 degrees a displacement field alone drives the nu=-2 trivial insulator into a pocket of incipient superconductivity - a sharp transition with a well-defined critical current that survives in-plane fields past four times the weak-coupling Pauli limit, though the resistance does not fall to zero

    [2026-09-25] · src Waleffe, Bhattacharyya, Kumar, Maginnis, Okounkova, Faehndrich, Watanabe, Taniguchi, Folk, Yankowitz; arXiv:2609.30202 (2026-09-24)

    • moire materials
    • chern insulators
    • superconductivity

    Moire graphene built from Bernal-stacked bilayer and trilayer sheets twisted against each other is a newer platform than the twisted-homobilayer systems that have dominated the field, and the authors state that superconductivity had not previously been seen in it except when a transition-metal-dichalcogenide layer supplies spin-orbit coupling by proximity. Waleffe et al. instead find, across twist angles from 1.05 to 1.50 degrees, Chern insulators at both integer and fractional moire filling for electron doping with Chern numbers reaching |C|3, tunable by twist angle and doping. At theta1.18 degrees, the trivial insulator at band filling nu=-2 is driven by displacement field alone - no TMD, no proximity coupling - into a pocket of incipient superconductivity: a sharp resistive transition with a well-defined critical current, persisting in an in-plane magnetic field to more than four times the weak-coupling Pauli limit, though the resistance does not fall fully to zero.

    Why

    The headline result is really two: a new moire graphene family with tunably high Chern number, and a route to superconductivity in that family that needs nothing beyond an applied displacement field to switch on, in contrast to every prior graphene-moire superconductor that has relied on twist-angle fine-tuning or an adjacent spin-orbit-coupling layer. The Pauli-limit violation is itself a clue about the pairing symmetry, pointing away from simple singlet pairing - but the resistance not reaching zero means this is a precursor state rather than an established superconductor, and the paper's own framing is that reducing disorder is now the open engineering question standing between "incipient" and a clean superconducting transition.

Music Practice

2

  1. 01

    Alto sax: fundamentals — crescendo off C, descending broken sixths

    [2026-09-25] · src —

    • alto
    • assignment

    Alto takes today's slot: three days since its last session on the 22nd is the longest gap of the three instruments right now, and trumpet went yesterday, so the two chops-dependent instruments don't land back to back. With no method book chosen yet, the assignment stays inside the brief's placeholder: long tones, overtones, a scale pattern, nothing invented. Today's fundamental is C, the next semitone above the B that crossed the break for the second time on 09-22 — a third straight session above it, so the octave-key handling is now the established default rather than a new demand. The warmup returns to crescendo attack, closing out the shape it left off with three sessions ago, and the musical target pushes the descending interval survey out to sixths.

    Warmup

    5 minutes: long tones on C and C♯, starting at pp and building a steady, controlled crescendo to f over eight counts, quarter=60, eight full counts per note. The target is a rise that stays centered in pitch the whole way up rather than sharpening as the air pressure builds — the same demand last tested on 09-13 and not since.

    Technical target

    Overtone series from fundamental C: voice up through C–C–G–C–E using only the (octave-key) C fingering, changing partials with throat and voicing, not embouchure — the same method as every prior session, now a third session running above the break. Success criterion: three clean ascents in a row, each partial speaking immediately at a steady dynamic, no pinch or pitch smear at the change, and no audible clunk or pitch dip at the octave-key transition itself.

    Musical target

    C major scale, one octave, in descending broken sixths from the top: 8–3, 7–2, 6–1 — the next interval size in the descending survey after thirds (09-16), fourths (09-19) and fifths (09-22), and the mirror image of 09-10's ascending broken sixths. Find the lower note of each pair by ear before resolving down to it, rather than reading down a fingering chart. Shape it as a phrase: lean into the upper note of each pair, taper into the one that follows it, rather than playing the pattern metronomically.

    Stop condition

    Stop the moment the crescendo starts sharpening instead of staying centered on the way up, or the octave-key transition starts needing a jaw shove or throat squeeze to speak cleanly. Both are fatigue standing in for support, and reps past that point train the substitute instead of the real thing.

  2. 02

    Listening: Charlie Parker, "Ko-Ko"

    [2026-09-25] · src —

    • alto
    • listening

    hearCharlie Parker — Ko-Ko · Tidal · Spotify

    Today's musical target asks for a descending sixth with no scalar approach — the lower note of each pair has to be found by ear and landed on directly, not read down to. "Ko-Ko" is built on exactly that kind of commitment: Parker's head over "Cherokee"'s changes, taken at a very fast tempo, moves in wide, decisive leaps rather than the stepwise runs bebop is more often remembered for, and none of them sound tentative or reached-for. Listen for how little the leaps interrupt the time feel — the line keeps moving at full speed through jumps that would make most players pause to reorient, which is the same commitment today's pattern is asking a single octave to hold onto.