Oxford Plasma
Theory Group welcomes applications for DPhil studies
and research in plasma physics in the areas of magnetic
confinement fusion (MCF) and plasma astrophysics
(including "laboratory astrophysics")
Note that the project descriptions given below are
not set in stone and we are willing to discuss modifications and
adjustments to them that might better reflect your interests and
inclinations. ***
NEW PROJECTS MAY APPEAR ON THIS PAGE IN DUE COURSE. COME
BACK AND CHECK! ***
Size of intake: this
depends on various hard-to-predict circumstances, in
particular funding arrangements; we accepted 2 fully funded
students in 2015, 4 in 2016, 3 in 2017, 3 in 2018, 1 in 2019,
3 in 2020, 2 in 2021, 1 in 2022, and 4 in 2023; we expect to
take at least 3 in 2024.
If you are interested in
MCF (either theoretical or experimental) or
generally in plasma physics, apply for a DPhil in Theoretical Physics.
Note that Theoretical Physics has three
separate DPhil competitions: in particle theory,
condensed matter and plasma physics. If you are
willing to be considered for more than one of these
topics, please state so explicitly in your
application form.
If you are interested in
plasma astrophysics, apply for a DPhil in Astrophysics. In order to be
considered by both subdepartments (Astrophysics and
Theoretical Physics) you may also apply for a DPhil in Theoretical Physics
(indicating plasma physics as your preferred area)
or, if you make a single application to either of
the two degrees, indicate clearly at the front
of your application form that you wish to be
considered by both subdepartments. This will
help us identify your application more quickly and
consider you for all available projects and funding
options across plasma physics. This is also a good
strategy if you are generally interested in plasma
physics and are flexible between its different
areas.
Internal Oxford scholarships: there
are a number of scholarships in physics available at
Oxford and its colleges. In order to be considered
for a scholarship funded by a particular college,
you do not need to select that college as your
college of first choice. There is one (known to us)
exception to this principle: if you are studying at
a Swiss university, apply to Lincoln
College to be eligible for a Berrow Foundation
Scholarship. If you are from India (or
certain other developing countries), make sure to
indicate on your application that you wish to be
considered for a Felix
Scholarship.
Choice of college: you may apply to
any college that accepts graduate applicants in
Physics. Choice of college can prove important for
your life as a graduate student: different colleges
offer different levels of support in terms of
research funds, accommodation, social integration
etc. We therefore recommend that you do not leave the
college choice blank, but do some research
on which college suits you best. We are happy to
give informal advice on the matter. Here is the list
of colleges where faculty members offering plasma
projects are Fellows: Merton (A. Schekochihin), LMH
(G. Gregori), Trinity
(A.
Bott), Univ (M. Barnes and P.
Norreys).
If you are considering
applying for an external
scholarship and require our endorsement, in
the first instance please contact the supervisor
with whom you are most interested in working. Note the opportunities for Commonwealth
Scholarships.
You are welcome to
address inquiries on science to any of the project
supervisors listed below and on the logistical
aspects of applying to Dr Derek
Hollman (but do please check first if your
question is perhaps already answered here).
At the application stage, you are not required to (although you
may if you wish) indicate which project you prefer --- we will
consider all applicants purely on intellectual merit. If you are
offered admission, we will strive to give you the opportunity to
work on the project of your choice.
Many current fusion
experiments rely on externally-applied, differential plasma
rotation to stabilise macroscopic instabilities and to
improve plasma confinement via the reduction of turbulent
transport. Sheared rotation may be even more important in
high-beta plasmas, where it appears to be crucial for
suppressing transport from kinetic-ballooning-mode
turbulence. However, in the large, dense plasmas envisioned
for next-generation experiments and reactors, the usual
techniques for rotating the plasma are unlikely to be
effective. It is thus critical to predict the level of
rotation in such plasmas and, likely, to develop alternative
methods of generating rotation. We propose to work with a
DPhil student to provide rotation predictions for high-beta
spherical tokamaks and to explore alternative strategies for
generating rotation. This work will build on previous
studies of intrinsic rotation in conventional tokamaks at
low beta. In particular, we will determine the amount of
rotation that could be generated with the modest applied
torques expected for a STEP-like device and then explore how
much rotation can be generated via use of up-down asymmetric
flux surface shapes, edge momentum input and other
"intrinsic" rotation mechanisms.
Electromagnetic (EM)
gyrokinetic (GK) turbulence in tokamaks, and the associated
transport of energy, particles, and momentum are not well
understood physically and are even less well parametrised
quantitatively, compared to the better known case of
electrostatic (ITG and ETG) turbulence. Even the nature of
the linear modes in this regime is an area where significant
contributions can still be made, and indeed have been made
recently [1-5]. Nonlinearly, a complex picture is emerging
whereby a transition from electrostatic to electromagnetic
regime occurs above a certain value of beta (ratio of
thermal to magnetic energy density) and leads to significant
enhancement of transport. This transition may be the culprit
for the unbounded growth of heat fluxes observed in GK
simulations of high-beta scenarios, in particular ones
envisioned for the operation of STEP. It is clear that, with
STEP and a number of other high-beta devices being
considered promising, and likely to be built, the EM
turbulence and transport must urgently be understood and
quantified. The student will join the existing collaborative
effort in this area between Oxford and Culham, and will
focus in particular on: (1) a comparative theory of MTM vs.
KBM/TAI/interchange transport in fusion plasma regimes
characteristic of MAST-U and STEP; (2) whether there exists
a (nonlinear) critical manifold in the parameter space that
separates high-transport EM regimes from low-transport
("Dimits-shifted") states: are there definite no-go zones?
are there sweet spots nearby? We shall also look at
strategies for testing theory and modelling prescriptions
using experimental output from MAST-U or NSTX---this would
present a unique opportunity to link the theory of EM
transport to the MAST-U programme and inform the design of
devices such as STEP.
1. D. Kennedy et al., "Electromagnetic gyrokinetic
instabilities in the Spherical Tokamak for Energy Production
(STEP), Part I: Linear physics and sensitivity," arXiv:2307.01670
2. M. Giacomin et al., "Electromagnetic gyrokinetic
instabilities in the Spherical Tokamak for Energy Production
(STEP), Part II: Transport and turbulence," arXiv:2307.01669
3. B. D. G. Chandran and A. A. Schekochihin, "The gyrokinetic
dispersion relation of microtearing modes in collisionless
toroidal plasmas," arXiv:2211.02103
4. T. Adkins et al., "Electromagnetic instabilities and plasma
turbulence driven by electron-temperature gradient," J. Plasma
Phys. 88, 905880410 (2022)
5. B. S. Patel et al., "Linear gyrokinetic stability of a high
beta non-inductive spherical tokamak," Nucl.
Fusion 62, 016009 (2022)
Future fusion power plants will
operate with a Deuterium-Tritium mixture that will produce
highly energetic alpha particles and neutrons as products
from the DT fusion reaction. The copious high-energy alpha
particles (3.5 MeV) will heat the rest of the plasma and
lead to a self-heating state, a burning plasma. These
conditions have not yet been achieved experimentally, and
there are serious questions on the extrapolations of the
existing models of turbulence to the burning regime,
particularly for spherical tokamaks. Highly energetic
particles are known to destabilise long-wavelength Alfven
waves in spherical tokamaks such as MAST-U and ST40, and
will certainly do so for ITER. There is growing experimental
and computational evidence that these waves on an
intermediate scale can mediate the small-scale turbulence
that governs the plasma confinement. Candidate explanations
for this could either be the generation of flows by the
Alfven waves, or the wave-wave nonlinear interaction. At
high plasma beta in machines such as STEP, the distinction
between electromagnetic turbulence and Alfven waves is
further blurred and the coupling between fast particles and
turbulence is more fundamental. This DPhil project will
focus on the following: (i) developing a theory of how
Alfven waves mediate turbulence in fusion plasmas; (ii)
estimating fast-particle population thresholds for the
interaction between Alfven waves and turbulence,
particularly for STEP conditions; (iii) comparing new
gyrokinetic computations with fluctuation measurements on
MAST-U.
Projects in
Plasma Astrophysics and Laser Plasmas
Candidates interested in any of these projects or generally
in plasma astrophysics, astrophysical turbulence and/or
dynamo theory are welcome to get in touch with prospective
supervisors for further information. A more bespoke project
can be designed to align with the inclinations and interests
of the student (for example how much emphasis is placed on
analytical vs. numerical methods or kinetic theory vs. fluid
dynamics, etc., is negotiable).
In magnetised astrophysical plasmas, there is a turbulent
cascade of electromagnetic fluctuations carrying free
energy from large to small scales. The energy is typically
extracted from large-scale sources (e.g., in the solar
wind, the violent activity in the Sun's corona; in
accretion discs, the Keplerian shear flow; in galaxy
clusters, outbursts from active galactic nuclei) and
deposited into heat---the internal energy of ions and
electrons. In order for this dissipation of energy to
happen, the energy must reach small scales---in weakly
collisional plasmas, these are small scales in the 6D
kinetic phase space, i.e., what emerges is large spatial
gradients of electric and magnetic fields and large
gradients of the particle distribution functions with
respect to velocities. This prompts two fundamental
questions: (1) how does the energy flow through the 6D
phase space and what therefore is the structure of the
fluctuations in this space: their spectra, phase-space
correlation functions etc. (these fluctuations are best
observed in the solar wind, but we can measure density and
magnetic fluctuations even in extragalactic plasmas, via
X-ray and radio observations); (2) when turbulent
fluctuations are dissipated into particle heat, how is
their energy partitioned between various species of
particles that populate the plasma: electrons, bulk ions,
minority ions, fast non-thermal particles (e.g., cosmic
rays). The latter question is particularly important for
extragalactic plasmas because all we can observe is
radiation from the particles and knowing where the
internal energy of each species came from is key to
constructing and verifying theories both of turbulence and
of macroscale dynamics and thermodynamics. This project
has an analytical and a numerical dimension (which of
these will dominate depends on the student's
inclinations). Analytically, we will work out a theory of
phase-space cascade at spatial scales between the ion and
electron Larmor scales. Numerically, we will simulate this
cascade using "gyrokinetic" equations---an approach in
which we average over the Larmor motion and calculate the
distribution function of "Larmor rings of charge" rather
than particles (this reduces the dimension of phase space
to 5D, making theory more tractable and numerics more
affordable).
Finally, with a theory of plasma turbulence in hand, it is
possible to attack what is probably the most fundamental
question of the field: in the absence of collisions, are
there universal equilibria, or classes of equilibria,
independent of initial conditions, that a turbulent plasma
will want to converge to? There is some recent progress
indicating that the answer is yes and that one predict
statistical-mechanically the emergence of universal
power-law (in particle energy) distributions---this is
exciting both on its own merits and because of the
astrophysical challenge of explaining theoretically
power-law distributions that are observed for, e.g.,
cosmic rays or solar-wind electrons. How to construct a
theory of that for a magnetised, turbulent plasma is an
open and exciting question. Attempting to do this will
again involve kinetic theory and/or kinetic simulations.
Background
Reading:
1. A. A. Schekochihin et al., "Astrophysical
gyrokinetics: kinetic and fluid turbulent cascades in
magnetized weakly collisional plasmas," Astrophys.
J.
Suppl. 182, 310 (2009)
2. A. A. Schekochihin et al., "Phase
mixing
vs. nonlinear advection in drift-kinetic plasma
turbulence,"
J.
Plasma Phys. 82, 905820212 (2016) (2019
IoP Payne-Gaposchkin Prize)
3. Y. Kawazura et al.,
"Thermal
disequilibration
of ions and electrons by collisionless plasma turbulence,"
PNAS 116, 771
(2019)
4. R.
Meyrand et al.,
"Fluidization
of collisionless plasma turbulence,"
PNAS 116, 1185
(2019)
5.
J. Squire et al.,
"High-frequency
heating of the solar wind triggered by
low-frequency turbulence,"
Nature
Astron. 6, 715 (2022)
6. R. J. Ewart et al., "Collisionless relaxation
of a Lynden-Bell plasma,'' J.
Plasma Phys. 88, 925880501 (2022)
7. R. J. Ewart et al., "Non-thermal particle
acceleration and power-law tails via relaxation
to universal Lynden-Bell equilibria," arXiv:2304.03715
One notable achievement of early 20th century physics was the
development and experimental validation of theories of the
material properties (such as thermal conductivity or
viscosity) of everyday gases. Today, there is a pressing need
to establish analogous theories for the material properties of
the magnetised, weakly collisional plasmas found in
inertial-confinement fusion (ICF) experiments [1,2] and also
in many extreme astrophysical environments [3]---for example,
the intracluster medium (ICM) of galaxy clusters or black hole
accretion flows. In ICF research, accurate modelling of heat
transport is crucial for realising high-yield target designs.
In astrophysics, material properties are thought to play a key
role in long-standing conundrums such as the ICM's anomalous
temperature profile. Correctly interpreting high-quality
astronomical observations of astrophysical systems (such as
the now-famous EHT image of the M87 black hole) also requires
a robust understanding of the underlying physics of the plasma
composing them. Yet astronomical observations and measurements
from laser-plasma experiments have shown that classical models
for the transport properties of magnetised, weakly collisional
plasmas often fail dramatically [4]. Thanks to recent
technological advances in both high-performance computing and
high-energy laser facilities, now is ideal for studying this
problem systematically, combining theory, simulations, and
experiments. During a project on this topic, a student would
focus on the design and subsequent delivery of a new
experiment that will characterise laser heating and thermal
conductivity in magnetised, weakly collisional plasma.
Measurements will then be directly compared to newly derived
models [5-7]. While it is intended that the project will be
experimentally focused, there is scope for the student to
pursue different aspects of the experiment depending on their
interests, including data analysis techniques and simulations.
Understanding cosmic magnetism is a long-standing
problem in astrophysics. Astronomical observations of
various astrophysical environments---for example,
those of our own galaxy by the MeerKAT telescope [1]
or of more distant galaxy clusters [2]---reveal the
presence of finely structured magnetic fields of
sufficient strength to affect the dynamics of such
systems. A possible mechanism for explaining the
presence and characteristics of these magnetic fields
is the so-called fluctuation dynamo, whereby
stochastic or turbulent motions of the plasma in which
these magnetic fields are embedded amplify and
maintain them [3]. The fluctuation dynamo has mostly
been studied using simplified magnetohydrodynamic
(MHD) plasma models whose key transport properties
(viz., resistivity and viscosity) do not depend on
macroscopic plasma properties such as density,
temperature, and the magnetic field. However, the
plasma often found in the astrophysical systems of
interest is often weakly collisional, and current
theories for the transport properties of such plasma
typically do predict a dependence on macroscopic
plasma properties. It is an outstanding question
whether "anomalous" transport properties can explain
why certain predictions of the simplified theory of
the fluctuation dynamo are at odds with astronomical
observations (for example, that the energy-containing
scale of the magnetic field is macroscopic). In this
project, a student would explore how more realistic
models of transport properties affect the fluctuation
dynamo using both theory and numerical simulations,
and then attempt to identify key differences with
simplified dynamo theories that could be detected in
astronomical observations.
There are a number of
possibilities within this project to design, take part in,
and theorise about laboratory experiments employing
laser-produced plasmas to model astrophysical phenomena and
basic, fundamental physical processes in turbulent plasmas.
Recent examples of our work in this field include turbulent
generation of magnetic fields ("dynamo") [1,2], supersonic
turbulence mimicking star-forming molecular clouds [3],
diffusion and acceleration of particles by turbulence [4,5],
suppression of thermal conduction in galaxy-cluster-like
plasmas [6]. Our group has access to several laser
facilities (including the National Ignition Facility, the
largest laser system in the world). Students will also have
access to a laser laboratory on campus, where initial
experiments can be fielded. Depending on the student's
inclinations, it is also possible to pursue a project
focused on theory and/or numerical modelling of plasma
phenomena in astrophysical and laboratory-astrophysical
environments.
Gamma-ray bursts (GRBs)
are among the most energetic events in the Universe. They
occur at cosmological distances and are the result of the
collapse of massive stars or neutron stars mergers, with
emission of relativistic "fireballs" of electron-positron
pairs. From astrophysical observations, a wealth of
information has been gleaned about the mechanism that
leads to such strong emission of radiation, with leading
models predicting that this is due to the disruption of
the beam as it blasts through the surrounding plasma. This
produces shocks and hydromagnetic turbulence that generate
synchrotron emission, potentially accelerating to
ultra-high energies the protons which are observed on
Earth as cosmic rays. However, there is no direct evidence
of the generation of either magnetic fields or cosmic rays
by GRBs. Estimates are often based on crude energy
equipartition arguments or idealized numerical simulations
that struggle to capture the extreme plasma conditions. We
propose to address this lacuna by conducting laboratory
experiments at large laser and accelerator facilities to
mimic the jet propagation through its surrounding plasma.
Such experiments will enable in situ measurement of the
plasma properties, with exquisite details that cannot be
achieved elsewhere. The experiments also complement
numerical simulations by providing long measurement times
extending into the non-linear regime where numerical
simulations are not possible today. The proposed
experiments will study fundamental physics processes,
unveil the microphysics of GRBs, and provide a new window
in high energy astrophysics using novel Earth-based
laboratory tools.
Background Reading:
1.
C. D. Arrowsmith et al., "Generating untradense pair
beams using 400 GeV/c protons," Phys. Rev. Res. 3, 023103 (2021)
Accreting supermassive
black holes (SMBHs) residing in active galactic nuclei
(AGN) at the centres of many galaxies, including our own,
are rightfully regarded as some of the most fascinating
and enigmatic objects in the Universe. These black holes,
and the powerful relativistic jets emanating from them,
often exhibit spectacular, violent phenomena, such as
bright high-energy flares with nonthermal X-ray and
gamma-ray spectra. They are also viewed as the most likely
generators of highly energetic non-electromagnetic
observational "messengers": extremely relativistic cosmic
rays and ultra-high-energy neutrinos, detected on Earth
with dedicated ground-based observatories. All these
observational signals indicate that BH environments are
very efficient relativistic particle accelerators.
Understanding how these cosmic accelerators work is an
outstanding problem in modern high-energy astrophysics.
Nonthermal particle acceleration is believed to be a
natural product of collective kinetic nonlinear plasma
processes, such as magnetic reconnection, shocks, and
magnetised plasma turbulence taking place in weakly
collisional plasmas. How these processes operate under the
extreme physical conditions expected in the exotic
relativistic plasma environments of accreting black holes
is, however, not well understood. The situation is greatly
complicated by special- and general-relativistic effects,
by strong interaction of the energetic emitting plasma
particles with radiation, and by quantum-electrodynamic
effects such as pair creation. Elucidating the complex
interplay of these effects with collective plasma
processes and, consequently, their impact on particle
acceleration is an active area of today's plasma
astrophysics research, presenting a number of interesting,
nontrivial theoretical challenges. This project will
address these fundamental plasma-theoretical questions and
their observational implications through a combination of
analytical and computational methods, with the balance
between theory and computation to be decided based on the
student's preferences.