TMO Standard Configuration
TMO Standard Configurations for Run 24
The Time-resolved Atomic, Molecular and Optical Science instrument (TMO) supports a wide range of science including gas phase photochemistry, attosecond electron dynamics, and the study of complex systems at the nanoscale. This includes the use of nonlinear and strong-field X-ray processes. The instrument features two interaction points appropriately named interaction point 1 (IP1) and interaction point 2 (IP2). TMO makes use of the LCLS soft X-ray undulators, providing horizontally polarized X-rays in the photon energy range from 250 eV to 1800 eV. During Run 24 TMO will offer two different end stations, the magnetic bottle time-of-flight electron spectrometer (MBES) and angle-resolving electron time-of-flight spectrometer (MRCO), in the first interaction point (IP1). At the second interaction point (IP2) we will offer our newly commissioned reaction microscope end station (DREAM).
Key Performance Parameters for Run 24
Run 24 will make use of the new superconducting LCLS-II accelerator which will eventually operate at repetition rates up to 1 MHz. You can find more information on the TMO beam line devices on our layout page. For more information on beamline devices or X-ray parameters available during Run 24, please contact James Cryan (jcryan@slac.stanford.edu).
X-ray Parameters
Repetition rate (Hz) | Up to 33 kHz, depending on machine performance | ||
---|---|---|---|
Energy Range (eV) | 200 - 1300 | ||
Pulse Duration | 20 fs (nominal) | Advanced Capabilities | |
Tunable to 5 fs | < 1 fs (XLEAP-II) | ||
Energy per pulse | > (160-60) µJ | Scales linear with | ~10 µJ |
Bandwidth (FWHM) | 0.5 % | 0.5 % | >1% |
Repetition rate (Hz) | > 30 kHz | > 30 kHz | > 10 kHz |
Spot Size, FWHM (range) | 1.0 - 200 um diameter | ||
Polarization | Linear, Horizontal | ||
Two Pulse Mode | < 10 µJ / pulse with tunable delay via split undulator method. |
The OPCPA laser system offers short (< 25 fs) 800 nm laser pulses. Harmonics of these pulses can be generated (400/266 nm).
Laser Parameters
Repetition rate (Hz) | Synchronized up to 33 kHz | |||
---|---|---|---|---|
Wavelength | 800 nm | 400 nm | 266 nm |
|
1300-2400 nm | ||||
Pulse Duration | < 25 fs | < 30 fs | < 30 fs | < 100 fs |
Energy per pulse (on target) | < 600 µJ | < 100 µJ | ~ 10 µJ | < 130 µJ (signal) |
Spot Size, FWHM (800 nm) | 50 to 100 um | |||
Polarization | Variable: linear, circular | |||
Angle | ~0.5o angle with X-ray beam | |||
Arrival Time Monitor | < 20 fs accuracy in X-ray/laser arrival time tagging should be available. Overall temporal resolution will be dependent on machine and instrument configuration |
For more information on the available laser parameters (and to discuss more advanced capabilities), please contact Mat Britton (matb@slac.stanford.edu) and James Cryan (jcryan@slac.stanford.edu).
MBES: Magnetic Bottle Electron Time-of-Flight Spectrometer in IP1
For Run 24 TMO will provide a magnetic bottle electron spectrometer. The spectrometer is coupled to a dual anode micro-channel plate detector allowing for some radial-discrimination of the measured spectrum.
The end station features:
- Gas targets:
- Either heated gas needle or
- In-vacuum oven
- 2m flight tube with retardation section, >50% collection efficiency
- Resolution DE/E <5%
- Retardation up to 200 eV
- Ion extraction plate and coincident Ion ToF capability
- Electron Detector
- The spectrometer is coupled to a dual anode micro-channel plate detector allowing for some radial-discrimination
- In Run 22 we will test a prototype time-resolving camera (TIXEL) for electron detection. We will try to make this detector available for Users in Run 23, but this detector will be offered at risk.
MRCO: Angle-resolving Electron Time-of-Flight Detector in IP1
In Run 24 TMO will provide and angular array of electron time-of-flight spectrometers offering high energy- and angular-resolution for electron spectroscopy. This end station features:
- Gas targets:
- Heated gas needle
- 16 eToF spectrometers, ~1% total collection efficiency
- Resolution DE/E < 1%
- Retardation up to 2000 eV
- Angular Acceptance 1.5o - 3.0o cone angle, per ToF
Photon Spectrometer Diagnostic
In Run 24 we will offer a photon spectral diagnostic downstream of IP1. This device uses an off-axis Fresnel Zone-Plate (FZP) to spectrally disperse the incident X-ray onto a high repetition rate detector. A line-scan camera at maximum repetition rate of ~100 kHz will be used to measure the single-shot spectra at the absorption edges of carbon, nitrogen, oxygen and neon elements. This compact photon spectrometer has a designed resolving power of ~1000 which we have demonstrated at the oxygen K-edge.
X-ray Parameters
Repetition rate (Hz) | Up to 33 kHz, depending on machine performance | ||
---|---|---|---|
Energy Range (eV) | 200 - 1300 | ||
Pulse Duration | 20 fs (nominal) | Advanced Capabilities | |
Tunable to 5 fs | < 1 fs (XLEAP-II) | ||
Energy per pulse | > (160-60) µJ | Scales linear with | ~10 µJ |
Bandwidth (FWHM) | 0.5 % | 0.5 % | >1% |
Repetition rate (Hz) | > 30 kHz | > 30 kHz | > 5 kHz |
Spot Size, FWHM (range) | 0.5 - 10 um diameter | ||
Polarization | Linear, Horizontal | ||
Two Pulse Mode | < 10 µJ / pulse with tunable delay via split undulator method. |
The Yb-based laser system will offer short (< 35 fs) 1030 nm laser pulses. Harmonics of these pulses can be generated (515/343/258 nm).
Laser Parameters
Repetition rate (Hz) | Synchronized up to 33 kHz | |||
---|---|---|---|---|
Wavelength | 1030 nm | 515 nm | 343 nm | 258 nm |
Pulse Duration | < 30 fs | < 40 fs | < 40 fs | < 40 fs |
Energy per pulse (on target) | > 700 µJ | > 200 µJ | > 50 µJ | >5 µJ |
Spot Size, FWHM (1030 nm) | 10 to 50 um | |||
Polarization | Variable: linear, circular | |||
Angle | co-linear with X-ray beam | |||
Arrival Time Monitor | < 20 fs accuracy in X-ray/laser arrival time tagging should be available. Overall temporal resolution will be dependent on machine and instrument configuration |
For more information on the available laser parameters (and to discuss more advanced capabilities), please contact Mat Britton (matb@slac.stanford.edu) and James Cryan (jcryan@slac.stanford.edu).
DREAM: Dynamic REAction Microscope at IP2
During Run 24 we will commission a reaction microscope spectrometer at the second interaction point in TMO. The standard configuration for Run 24 features ion detection with a 120 mm Hexanode delay-line detector. Electron detection is not part of the standard configuration and will be offered (at-risk). This end station features:
- Gas Targets:
- Skimmed molecular beam source
- Charged Particle Detection:
- 5 cm, short arm spectrometer (electron/ high-energy ions)
- 27 cm, long arm spectrometer (lower energy ions)
- Dual 120 mm Hexanode delay-line detectors.
- Standard Configuration: Ions-only, either with long or short spectrometer.
Not Planned for Run 24
- Double-sided VMI in LAMP (dVMI)
- Co-axial VMI (cVMI)
- Kaesdorf Electron Spectrometer
- Photon Imaging Detectors
Non-Standard Configurations
For non-standard configuration or more information contact James Cryan (jcryan@slac.stanford.edu).
TMO INSTRUMENT TEAM
James Cryan
TMO Instrument Lead Scientist
(650) 926-3290
jcryan@slac.stanford.edu
Justin James
Beamline Engineer
(650) 926-3842
jhjames@slac.stanford.edu
Ming-Fu Lin
TMO Scientist
(650) 926-2586
mfucb@slac.stanford.edu
Razib Obaid
TMO Scientist
robaid@slac.stanford.edu
Thomas Wolf
TMO Scientist
(650) 926-2533
thomas.wolf@slac.stanford.edu
Taran Driver
TMO Scientist
tdd14@slac.stanford.edu
Xiang Li
TMO Scientist
xiangli@slac.stanford.edu
Mike Glownia
Laser Scientist
jglownia@slac.stanford.edu
Ruaridh Forbes
Laser Scientist
ruforbes@slac.stanford.edu
Mat Britton
Laser Scientist
matb@slac.stanford.edu
Jeff Aldrich
Area Manager
jaldrich@SLAC.Stanford.EDU