"Diffraction before destruction" — X-ray free-electron laser pulses outrun radiation damage in a stream of protein nanocrystals
Serial femtosecond crystallography (SFX) begins with a deceptively simple engineering problem: how do you deliver a continuous, unbroken stream of micron- and sub-micron-scale protein crystals across an X-ray beam, one at a time, without clogging, without crystallizing in air, and fast enough to keep pace with pulses arriving up to 27,000 times per second? The answer — the gas dynamic virtual nozzle — is one of the quiet mechanical triumphs that made XFEL crystallography possible.
The GDVN (DePonte et al., 2008) injects a liquid suspension of crystals through a fine glass capillary, then focuses it with a coaxial sheath of helium or nitrogen gas flowing at high velocity. The gas accelerates and compresses the liquid into a jet far thinner than the capillary orifice itself — typically 1–10 µm in diameter — hence "virtual" nozzle: the effective aperture is smaller than any physical opening, so it never clogs on crystals passing through it.
The jet travels continuously through vacuum or a helium-filled interaction chamber, crossing the XFEL focus at a fixed point. Because the jet runs continuously rather than being triggered pulse-by-pulse, the vast majority of the liquid — and the crystals in it — never encounters an X-ray pulse at all and is simply discarded. This is the central inefficiency of classic SFX: at 120 Hz with a jet velocity of tens of m/s, only a tiny fraction of injected crystals are ever hit.
Many of the most biomedically important protein targets — G-protein-coupled receptors (GPCRs), photosynthetic reaction centers, membrane transporters — stubbornly refuse to form the large, well-ordered crystals (tens to hundreds of microns) that conventional synchrotron crystallography demands. They often crystallize only as microcrystalline showers: vast numbers of nano- to micro-crystals, each too small and too radiation-sensitive to survive a conventional rotation-method X-ray dataset, but individually perfectly good diffractors for a single femtosecond exposure.
Sample delivery for these fragile crystal slurries typically uses lipidic cubic phase (LCP) injectors — a viscous, gel-like medium in which membrane protein crystals grow directly and which can be extruded at a much slower, gentler flow rate than a pure liquid jet, dramatically reducing sample consumption.
Because liquid jets waste so much sample between pulses, several alternative delivery schemes have been developed to match sample supply to pulse arrival:
• Fixed-target scanning: crystals are spotted onto a thin silicon or polymer chip in a grid pattern, and the chip is stepped through the beam synchronously with each pulse — essentially zero waste between shots. • Drop-on-demand injectors: piezoelectric dispensers eject a single droplet containing one crystal exactly when a pulse is due, timed to the accelerator clock. • High-viscosity extrusion (LCP, agarose, grease matrices): slow continuous ribbons that conserve precious membrane-protein sample.
The choice of delivery method is one of the most consequential experimental design decisions in SFX, trading off sample consumption, background scatter, and achievable hit rate.
A full high-resolution SFX dataset can require millions of individual crystals — yet because each crystal is only microns across, an entire dataset can still be collected from just a few milligrams of purified, crystallized protein.
An X-ray free-electron laser is not a conventional light source scaled up — it is a fundamentally different way of making X-rays. Relativistic electron bunches, accelerated to gigaelectronvolt energies down kilometers of linear accelerator, are forced through long undulator magnets where they self-organize into micro-bunches that radiate coherently, producing pulses of X-rays billions of times brighter than any synchrotron, compressed into a burst lasting only femtoseconds.
In a conventional laser, photons bounce between mirrors and stimulate identical photons from a gain medium. An XFEL has no mirrors that could survive its intensity, and no atomic gain medium — instead it uses SASE. A bunch of electrons, initially radiating incoherently as they wiggle through an undulator's alternating magnetic field, interacts with its own emitted radiation. Electrons that happen to be slightly ahead in phase are decelerated, those behind are accelerated, and over tens to hundreds of meters of undulator this feedback organizes the electron bunch into thin microbunches spaced exactly one X-ray wavelength apart.
Once microbunched, the electrons radiate coherently — in phase — and the X-ray intensity grows exponentially along the undulator until it saturates. The result is a pulse of transversely and (mostly) longitudinally coherent X-rays with peak power in the tens of gigawatts, self-organized entirely from noise rather than seeded by an external laser.
Two properties combine to make diffraction-before-destruction possible: extreme peak brightness and extreme pulse brevity. The instantaneous X-ray flux at the sample is so high that even a single micron-scale nanocrystal — far too small to give a measurable signal from a conventional lab or even synchrotron source in any reasonable exposure — scatters enough photons in one shot to record a usable diffraction pattern.
Critically, that entire pulse arrives and is gone in ~10–50 femtoseconds — shorter than the time it takes atoms in the crystal to move appreciably, and far shorter than the timescale on which the deposited energy can propagate into structural damage. The femtosecond pulse duration is not a byproduct of the SASE process; it is the property that makes the whole "diffract-before-destroy" strategy work.
A handful of facilities worldwide operate hard X-ray FELs capable of macromolecular SFX, each with a different accelerator technology and repetition rate:
• LCLS (Linac Coherent Light Source, SLAC, USA) — the first hard X-ray FEL, operational since 2009, historically pulsed at 120 Hz using a copper linac; upgraded (LCLS-II) with a superconducting linac reaching up to 1 MHz. • European XFEL (Hamburg, Germany) — superconducting linac delivering pulse trains at up to 27,000 Hz (27 kHz), the highest average repetition rate of any hard X-ray FEL. • SACLA (Japan) — compact copper-linac FEL operating at up to 60 Hz–120 Hz, known for very short pulses and a compact accelerator footprint. • PAL-XFEL (Pohang, South Korea) — a newer copper-linac facility operating around 60 Hz-scale repetition rates with a design closely related to LCLS.
The shift from 120 Hz to multi-kHz and MHz repetition rates over the past decade is the single biggest driver of faster, cheaper SFX datasets — turning experiments that once took days of beamtime into ones completed in minutes.
The European XFEL's 27,000 Hz repetition rate means it can, in principle, deliver as many X-ray pulses in under five seconds as the original LCLS delivered in a full minute at 120 Hz — a step change in how fast a serial dataset can be assembled.
Every X-ray crystallography experiment is, at some level, a race between the useful scattering signal and the radiation damage the same X-rays inflict on the sample. XFEL serial femtosecond crystallography wins that race in the most extreme way possible: by making the exposure so short that the crystal has no time to respond before the data is already recorded — the destruction happens, but only after the picture has been taken.
Before any XFEL capable of macromolecular crystallography existed, physicist Richard Neutze and colleagues published a theoretical paper in Nature (2000) proposing that a sufficiently intense, sufficiently short X-ray pulse could record a diffraction pattern from a single macromolecule or nanocrystal before radiation damage destroyed the sample's structural integrity. Their molecular dynamics simulations showed that atoms in a radiation-ionized sample remain close enough to their original positions for tens of femtoseconds — even as the sample begins to explode from the resulting Coulomb repulsion between ionized atoms — for a pulse of that duration to still capture an essentially undamaged diffraction pattern.
The proposal was radical: rather than trying to minimize radiation dose per exposure (the entire strategy of conventional cryo-crystallography), embrace an enormous dose delivered so quickly that the physical consequences simply have not happened yet by the time the scattered photons have left the sample.
The principle remained untested until the LCLS came online. In 2011, Henry Chapman and a large international collaboration published the first experimental demonstration in Nature, streaming a suspension of lysozyme nanocrystals across the LCLS beam using an early gas dynamic virtual nozzle and recording thousands of single-shot diffraction patterns, each from a crystal annihilated by the very pulse that produced its pattern.
By merging thousands of these single-shot "diffract and destroy" patterns from randomly oriented crystals, the team reconstructed a structure of lysozyme at room temperature with no measurable radiation-damage artifacts — proving that Neutze's decade-old theoretical prediction held up in the real world, and launching serial femtosecond crystallography as a practical structural biology method.
In the 2011 proof-of-principle experiment, each lysozyme nanocrystal absorbed a radiation dose roughly 1,000 times higher than the dose that would destroy a crystal in a conventional synchrotron experiment — and still yielded an undamaged diffraction pattern, because the pulse was over before the damage could manifest structurally.
When the femtosecond pulse strikes the crystal, its photons are absorbed primarily by photoionization, ejecting core electrons from atoms and leaving behind a cascade of positively charged ions. This sudden, localized ionization creates immense electrostatic repulsion between neighboring atoms — the sample is, in effect, instantaneously turned into a small plasma that then violently disassembles: the "Coulomb explosion."
The key timescale separation is this: photoionization and the scattering event that produces the diffraction pattern happen essentially instantaneously, within the ~10–50 fs pulse envelope. Nuclear motion — atoms actually displacing from their crystallographic positions in response to that ionization — takes tens to hundreds of femtoseconds to become significant, and the crystal's visible physical disintegration unfolds over picoseconds to microseconds afterward. The diffraction pattern is recorded during the brief window in which the electron density is still essentially undisturbed, even though the fate of every atom in the crystal has already been sealed.
Because every crystal is annihilated after exactly one exposure, an SFX experiment cannot rotate a single crystal through a data collection wedge the way conventional crystallography does. Instead it collects one still, randomly oriented diffraction "snapshot" per crystal, and repeats this hundreds of thousands to millions of times — a fundamentally statistical approach to structure determination that depends on fast, automated hit-finding to separate signal from an ocean of empty frames.
In rotation-method crystallography, one crystal is mounted, cooled, and rotated through the beam over minutes to hours, building a complete 3D dataset from thousands of finely spaced still images of the same crystal at known, closely-spaced orientations. SFX cannot do this: the crystal is gone after a single pulse. Every frame comes from a different crystal, in a completely random, a priori unknown orientation, with a random position offset relative to the beam focus (partiality) and often a randomly varying crystal size.
The experiment therefore becomes fundamentally serial and statistical: instead of few crystals sampled finely, use many thousands of crystals sampled once each, and rely on the sheer number of random orientations to eventually cover all of reciprocal space needed to reconstruct the full 3D structure.
At any given moment, most pulses arriving at the interaction point find nothing but liquid — no crystal happens to be present at the focus when the X-rays arrive. These "miss" frames record only weak background scatter from the liquid jet and must be discarded automatically, since manual inspection of millions of frames is impossible.
Software such as CrystFEL's peakfinder8 algorithm (part of the broader Cheetah/CrystFEL processing pipeline) scans every detector frame in real time (or near-real time) for the sharp, localized Bragg peaks characteristic of crystalline diffraction, distinguishing them from the smooth, diffuse background of an empty shot. Frames exceeding a minimum peak count are flagged as "hits" and passed on for indexing; the rest are discarded. Typical hit rates range from a few percent up to ~30%, depending heavily on crystal density in the jet, crystal size, and jet-beam timing overlap.
Each hit frame is a single still diffraction pattern from a crystal in an unknown 3D orientation, intersecting the Ewald sphere at a random offset — meaning most Bragg reflections are only partially recorded ("partials") rather than fully integrated as they would be across a fine rotation series. Indexing algorithms (built into CrystFEL, using methods such as DirAx, MOSFLM, or XGANDALF) must determine the crystal's orientation and unit cell from this single partial pattern alone, frame by frame, with no information carried over from one crystal to the next.
Only a fraction of hits successfully index — typically 30–80% depending on crystal quality and diffraction resolution — meaning that of, say, 50,000 hit frames, perhaps 20,000–40,000 contribute usable, oriented partial-reflection data to the final merge.
The final step of SFX turns a mountain of partial, randomly oriented single-crystal snapshots into a single coherent 3D electron density map. Because no individual pattern contains complete information, structure determination becomes a large-scale statistical merging problem — one that, once solved, unlocks structures and dynamics inaccessible to any other crystallographic method.
Because each indexed hit frame records only a random partial slice through reciprocal space, no single pattern — or even a modest number of them — provides complete, correctly scaled reflection intensities. SFX instead relies on the Monte Carlo integration approach pioneered for serial crystallography: pool observations of the same reflection across tens to hundreds of independent, randomly oriented crystals, and let the partiality and scaling errors of individual observations average out statistically as the number of independent measurements grows.
Tools such as CrystFEL's partialator program refine per-crystal scaling factors and partiality models against the growing merged dataset iteratively, converging on a self-consistent set of fully integrated structure-factor amplitudes. In practice this means the quality of an SFX structure improves not by exposing a crystal longer or harder — impossible, since each is destroyed instantly — but by collecting more independent crystal snapshots.
SFX opened structural biology to targets that had long resisted conventional synchrotron crystallography:
• Membrane proteins and GPCRs: G-protein-coupled receptors and other membrane proteins frequently yield only microcrystalline showers grown in lipidic cubic phase, far too small and fragile for rotation-method data collection, but ideal for room-temperature SFX. • Radiation-damage-free structures: because each crystal is destroyed by the very pulse that measures it, SFX structures are free of the specific radical-mediated radiation damage (disulfide bond breakage, metal center reduction, decarboxylation) that accumulates during conventional, longer synchrotron exposures — important for accurately visualizing metalloenzyme active sites and redox-sensitive cofactors. • Room-temperature structures: unlike cryocrystallography, SFX crystals are typically measured near physiological temperature, avoiding potential cryo-cooling artifacts in protein conformation.
The single most transformative application of SFX is time-resolved crystallography: because a fresh crystal is delivered for every single shot, each one can be triggered by an optical "pump" laser pulse a precisely controlled delay before the X-ray "probe" pulse arrives, then discarded. Repeating this at thousands of different, systematically varied time delays — femtoseconds to milliseconds apart — and merging each delay point's patterns separately produces a stop-motion "molecular movie" of a light-triggered reaction unfolding in real time.
Landmark examples include watching Photosystem II's oxygen-evolving complex step through the catalytic S-state cycle of water oxidation, tracking the light-driven proton pumping cycle of bacteriorhodopsin, and capturing the earliest femtosecond photoisomerization steps of rhodopsin as it initiates the visual phototransduction cascade — dynamics far too fast and far too radiation-sensitive to observe by any other structural method.
Pump-probe SFX has captured the retinal chromophore in rhodopsin beginning to isomerize within femtoseconds of absorbing a photon — the literal first structural step of vertebrate vision, resolved directly in atomic detail.
| Product | Indication | Trial Design | Key Result |
|---|---|---|---|
| Synchrotron rotation crystallography | Large, well-ordered single crystals (>10–20 µm), radiation-tolerant samples | Continuous monochromatic beam, fine-sliced rotation of one cryocooled crystal | Highest routine resolution, mature and inexpensive pipeline |
| XFEL Serial Femtosecond Crystallography | Nanocrystals/microcrystals, radiation-sensitive or hard-to-grow proteins, reaction dynamics | Femtosecond pulses, diffraction-before-destruction, serial single-shot Monte Carlo merging | Room-temperature, radiation-damage-free, enables femtosecond time-resolved movies |
| Cryo-EM (single-particle) | Large complexes and membrane proteins, no crystal required at all | Vitrified single particles imaged directly; thousands of particle images averaged computationally | No crystallization needed, rapidly improving near-atomic resolution |
| Room-temperature serial synchrotron (SSX) | Microcrystals measurable at synchrotron sources | Fast-readout pixel detectors, fixed-target or jet delivery, modest dose split across many crystals | Near-physiological temperature and serial statistics without requiring an XFEL |