Beam-beam compensation scheme doubles proton-proton collision rates at RHIC

Beam-beam compensation scheme doubles proton-proton collision rates at RHIC
Brookhaven Lab accelerator physicist Wolfram Fischer stands next to the electron lensing apparatus at the Relativistic Heavy Ion Collider (RHIC), a particle accelerator/collider at the US Department of Energy's Brookhaven National Laboratory. Credit: Brookhaven National Laboratory

Accelerator physicists at the U.S. Department of Energy's (DOE) Brookhaven National Laboratory have successfully implemented an innovative scheme for increasing proton collision rates at the Relativistic Heavy Ion Collider (RHIC). More proton collisions at this DOE Office of Science User Facility produce more data for scientists to sift through to answer important nuclear physics questions, including the search for the source of proton spin.

"So far we have doubled the peak and average 'luminosity'-measures that are directly related to the collision rates," said Wolfram Fischer, Associate Chair for Accelerators of Brookhaven's Collider-Accelerator Department and lead author on a paper describing the success just published in Physical Review Letters. And, he says, there's potential for further gains by increasing the number protons from the injectors even more.

Colliding polarized protons

RHIC is the world's only polarized proton collider, capable of sending beams of protons around its 2.4-mile-circumference racetrack with their internal magnetic axes (also known as spins) aligned in a chosen direction. Colliding beams of such "spin polarized" protons and manipulating the spin directions gives scientists a way to explore how their internal building blocks, quarks and gluons, contribute to this intrinsic particle property.

Data at RHIC have revealed that both quarks and gluons make substantial contributions to spin, but still not enough to explain the total spin value. More data will help resolve this spin mystery by reducing uncertainties and allowing nuclear physicists to tease out other unaccounted for contributions.

Beam-beam compensation scheme doubles proton-proton collision rates at RHIC
A schematic layout of electron lens components. An electron gun creates a low-energy electron beam that is transported into a superconducting magnet where the magnetic field keeps the electrons from being deflected by the more energetic protons circulating in RHIC. As the protons pass through the negatively charged electron beam, they experience a kick that compensates for the repulsive positive charge of the oncoming proton beam. These kicks nudge the protons toward the center of the beam to maximize proton collision rates. Credit: Brookhaven National Laboratory

But getting more protons to collide is an ongoing challenge because, as one beam of these positively charged particles passes through the other, the particles' like charges make them want to move away from one another.

"The strongest disturbance a proton experiences when it travels around the RHIC ring is when it flies through the other ," Fischer said. "The result of the positive charges repelling is that the protons get deflecting kicks every time they fly through the oncoming beam."

Opposite charge produces opposite push

The size of the repulsive kick depends on where the proton flies through the beam, with protons about halfway from dead center to the outside edge of the beam's cross-section experiencing the largest outward push. Particles closer to the center or the outer edge of the cross-section experience less repulsion.

Because of the variable shape of this effect-increasing to a peak and then decreasing with distance from the beam's center-it's impossible to correct using magnets. "The magnetic field strength in magnets increases steadily from the center out," Fischer said.

Beam-beam compensation scheme doubles proton-proton collision rates at RHIC
The electron lensing team is (front row, left to right): Xiaofeng Gu, Peter Thieberger, Wolfram Fischer, Zeynep Altinbas, Yun Luo, (back, l to r) Chuyu Liu, Alexander Pikin, Al Marusic, Jon Hock, Mike Costanzo. Additional co-authors on the electron lensing paper not shown: Rob Michnoff, Toby Miller, Vincent Schoefer, and Simon White. Credit: Brookhaven National Laboratory

So instead, the scientists turned to using oppositely charged particles to produce a compensating push in the opposite direction.

"We've implemented electron lensing technology to compensate for these head-on beam-beam effects," Fischer said.

Essentially, they use an electron gun to introduce a low-energy into a short stretch of the RHIC accelerator. Within that stretch, the electrons are guided by a magnetic field that keeps them from being deflected by the more . As the protons pass through the negatively charged electron beam, they experience a kick in the opposite direction from the repulsive positive charge, which nudges the protons back toward the center of the beam.

"It's not a glass lens like you'd find in a camera," Fischer said, "but we call the technique 'electron lensing' because, like a lens that focuses light, the electron beam changes the trajectory of the protons flying through it."

Riding the optical wave

The scientists also take advantage of certain "optical" properties of RHIC's particle beams to ensure the method's efficacy.

"Ideally you would like to produce these compensating pushes right where the collisions happen, within the STAR and PHENIX detectors," Fischer said. "But then the experiments wouldn't work anymore. So we placed the electron lenses, one on each beam, at a certain distance from the detectors-called the optical distance-where they have an effect at the same point in the 'phase' of the particle beam that's inside the detectors."

Like a wave of light or sound that oscillates up and down in amplitude at a given frequency, the particles that travel around RHIC also oscillate a tiny bit. As long as the nuclear physicists know the frequency of the oscillations and give their electron-lensing kicks at the same point in that oscillation that the particles reach within the detector, the effect will compensate for the proton repulsion the particles experience at that distant location.

So far, the scientists have doubled the proton-proton collision rates at RHIC. They could potentially get even higher gains by increasing the number of injected into the machine.

"The key challenge will be to maintain the high degree of polarization the experiments need to explore the question of ," Fischer said. But he insists there is clear potential for even higher proton-proton luminosity.


Explore further

Relativistic Heavy Ion Collider smashes record for polarized proton luminosity

More information: W. Fischer et al. Operational Head-on Beam-Beam Compensation with Electron Lenses in the Relativistic Heavy Ion Collider, Physical Review Letters (2015). DOI: 10.1103/PhysRevLett.115.264801
Journal information: Physical Review Letters

Citation: Beam-beam compensation scheme doubles proton-proton collision rates at RHIC (2016, January 4) retrieved 19 July 2019 from https://phys.org/news/2016-01-beam-beam-compensation-scheme-proton-proton-collision.html
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Jan 04, 2016
That's a really clever way to compensate!

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