Skip to main content
Sandbox Physics
Molecules, forces and ultrafast dynamics

Apparatus · Observation · Inference

Attosecond pulses: a broad spectrum still needs a clock

Sandbox Physics ·

How did electron spectra establish a pulse train or an isolated pulse shorter than a femtosecond?

  1. High-harmonic generation
  2. XUV and delayed infrared field
  3. Photoelectron energy-delay data
  4. Infer phase and duration
RABBIT pulse-train metrology and isolated-pulse streaking use different observables and reconstruction assumptions.

The harmonics supplied bandwidth, not a stopwatch

High harmonics generated in gases provided extreme-ultraviolet bandwidth associated with very short timescales. L’Huillier’s work helped establish and understand that source. A wide spectrum, however, can form a short burst, a train, or a longer chirped field depending on relative spectral phases.

The 2023 scientific background distinguishes the generation work from the 2001 metrology demonstrations. Agostini’s group characterized a train with roughly 250-attosecond bursts; Krausz’s group characterized an isolated pulse. Those are distinct temporal structures, not interchangeable records of one pulse.

Sources: [2][4]

RABBIT compares two routes to a sideband

An XUV harmonic plus absorption or emission of an infrared photon can reach the same final electron energy as a neighboring harmonic with the opposite infrared exchange. The paths interfere. Scanning delay modulates the sideband and constrains relative phases between neighboring harmonics.

The signal includes both XUV spectral phase and atomic two-photon phase. A measured phase is therefore not automatically a pure source emission time. The pulse-train reconstruction needs the harmonic amplitudes and the stated phase corrections or approximations.

Sources: [2][4][5]

Streaking uses a field that changes after release

For an isolated XUV burst, a synchronized infrared field changes the final photoelectron momentum according to release time. Measuring energy against delay converts timing information into a spectrogram. Hentschel and coauthors’ abstract reports a soft-X-ray duration of 650 attoseconds with an uncertainty of 150 attoseconds.

In a simple classical propagation limit, final momentum differs from the initial momentum by the vector potential at release, with the sign set by electron charge. The expression below uses negative electron charge and a vector potential vanishing after the pulse. Coulomb and scattering effects require additional treatment.

pf≃p0−eA(t0),e>0\mathbf p_f\simeq\mathbf p_0-e\mathbf A(t_0),\qquad e>0

Sources: [3][2]

A pulse duration is an inferred quantity

Neither method photographs an electron orbit frame by frame. A duration follows from a measurement model applied to energy-delay data, with assumptions about the target, dressing field and retrieval. Different phase conventions and atomic responses matter when comparing reported delays.

CPA prepares an intense short driver, but it is not itself high-harmonic phase measurement or attosecond reconstruction. A femtosecond source Lab cannot be counted as a completed attosecond metrology instrument.

Sources: [2][3][1][5]

Read a spectrogram before the reconstructed pulse

Keep the sideband oscillation or streaking trace beside the claimed temporal result, and identify which atomic phase or propagation approximation was used. The linked CPA model explains the driver preparation only; this reading path explicitly leaves the independent metrology task separate.

Sources: [2][3]

Sources and reading notes

Read sources: the Academy’s indexed scientific-background passages, the CEA experimental team’s account, Hentschel’s author abstract and the Dahlström–L’Huillier–Maquet author abstract on measurement-induced phase. The full official background PDF was inaccessible; reported durations are attributed measurements, not an independent reanalysis.

  1. D. Strickland, Generating High-Intensity Ultrashort Optical Pulses (2018), original CPA apparatus passage

    Indexed author passage read: fibre broadening/stretching, Nd:glass amplification and grating compression. Full lecture endpoint returned 403.

  2. Royal Swedish Academy of Sciences, Scientific Background: Physics Prize 2023, generation and metrology sections

    Indexed scientific-background passages read: HHG, RABBIT pulse trains and isolated-pulse streaking. Official PDF returned 403; this is an institutional retrospective.

  3. M. Hentschel et al., Attosecond metrology, Nature414,509–513 (2001)

    Author abstract read, including 650 attoseconds with 150-attosecond uncertainty; full publisher article not used.

  4. CEA attophysics team, Femtosecond–attosecond physics and chemistry: original pulse-train account

    Team’s primary account read: 2001 RABBITT characterization of 250-attosecond bursts and later harmonic-phase/chirp measurements.

  5. J. M. Dahlström, A. L’Huillier & A. Maquet, Introduction to attosecond time-delays in photoionization (2012), author abstract

    Author abstract read: observed delay includes a measurement-induced continuum–continuum phase, rather than only single-photon ionization delay. Full tutorial not claimed as read.

FeedbackSomething broken, confusing, or missing on this page?Tell us
What kind of feedback?

Sent with this page’s address, its Lab ID, the site language and your device type. Please leave out personal details. Feedback is kept for up to 12 months.Privacy policy