Gia Dvali’s research while affiliated with Arnold Arboretum, Harvard University and other places

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Publications (261)


FIG. 5: An example of a diagram generating the neutron-antineutron transition.
FIG. 6: A schematic representation of correlations between various experimental searches.
TeV Window to Grand Unification: Higgs's Light Color Triplet Partner
  • Preprint
  • File available

November 2024

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6 Reads

Gia Dvali

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Otari Sakhelashvili

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Anja Stuhlfauth

The color-triplet partner of the Higgs doublet, called a T-particle, is a universal feature of Grand Unification. It has been shown some time ago that this particle can be accessible for direct production in collider experiments. In this paper we point out that the T-particle represents a simultaneous low-energy probe of baryon number violation as well as of the origin of the neutrino mass, linking the mediation of proton decay with oscillations of the neutron into a sterile neutrino. We point out a triple correlation between its collider signatures, proton decay measurements and the searches for the magnetic resonance disappearance of free neutrons in cold neutron experiments. In this way, the T-particle can provide a diversity of correlated experimental windows into Grand Unification.

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Coherent States in Gauge Theories: Topological Defects and Other Classical Configurations

November 2024

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6 Reads

We present a formulation of coherent states as of consistent quantum description of classical configurations in the BRST-invariant quantization of electrodynamics. The quantization with proper gauge-fixing is performed on the vacuum of the theory, whereas other backgrounds are obtained as BRST-invariant coherent states. One of the key insights is the possibility of constructing the coherent states of pure-gauge configurations. This provides a coherent state understanding of topologically non-trivial configurations in gauge theories, and makes number of features, such as the suppression of transitions between topologically-distinct sectors, very transparent at full quantum level. As an example, we construct the Nielsen-Olesen string as a BRST-invariant coherent state. The Abelian pure-gauge configurations can also be viewed as useful analogs for a set of space-times related by coordinate reparameterizations in General Relativity.


First mechanical realization of a tunable dielectric haloscope for the MADMAX axion search experiment

November 2024

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6 Reads

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1 Citation

Journal of Instrumentation

B. Ary Dos Santos Garcia

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D. Bergermann

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A. Caldwell

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[...]

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MADMAX, a future experiment to search for axion dark matter, is based on a novel detection concept called the dielectric haloscope. It consists of a booster composed of several dielectric disks positioned with μm precision. A prototype composed of one movable disk was built to demonstrate the mechanical feasibility of such a booster in the challenging environment of the experiment: high magnetic field to convert the axions into photons and cryogenic temperature to reduce the thermal noise. It was tested both inside a strong magnetic field up to 1.6 T and at cryogenic temperatures down to 35 K. The measurements of the velocity and positioning accuracy of the disk are shown and are found to match the MADMAX requirements.


Hint to supersymmetry from the GR vacuum

October 2024

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11 Reads

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1 Citation

Physical Review D

The S -matrix formulation of gravity suggests that the θ -vacuum structure must not be sustained by the theory. We point out that, when applied to the vacuum of general relativity, this criterion hints to supersymmetry. The topological susceptibility of gravitational vacuum induced by Eguchi-Hanson instantons can be eliminated neither by spin- 1 / 2 fermions nor by an axion coupled via them since such fermions do not provide instanton zero modes. Instead, the job is done by a spin- 3 / 2 fermion, hence realizing a local supersymmetry. This scenario also necessitates the spontaneous breaking of supersymmetry and predicts the existence of axion of R symmetry which gets mass exclusively from the gravitational instantons. The R axion can be a viable dark matter candidate. Matching between the index and the anomaly imposes a constraint that spin- 1 / 2 fermions should not contribute to the chiral gravitational anomaly. Published by the American Physical Society 2024


Consistent Canonical Quantization of Gravity: Recovery of Classical GR from BRST-invariant Coherent States

September 2024

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1 Read

We perform canonical quantization of General Relativity, as an effective quantum field theory below the Planck scale, within the BRST-invariant framework. We show that the promotion of constraints to dynamical equations of motion for auxiliary fields leads to the healthy Hamiltonian flow. In particular, we show that the classical properties of Einstein's gravity, such as vanishing Hamiltonian modulo boundary contribution, is realized merely as an expectation value in appropriate physical states. Most importantly, the physicality is shown not to entail trivial time-evolution for correlation functions. In the present approach we quantize the theory once and for all around the Minkowaski vacuum and treat other would-be classical backgrounds as BRST-invariant coherent states. This is especially important for cosmological spacetimes as it uncovers features that are not visible in ordinary semi-classical treatment. The Poincar\'e invariance of the vacuum, essential for our quantization, provides strong motivation for spontaneously-broken supersymmetry.


First search for axion dark matter with a Madmax prototype

September 2024

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16 Reads

This paper presents the first search for dark matter axions with mass in the ranges 76.56 to 76.82 μ\mueV and 79.31 to 79.53 μ\mueV using a prototype setup for the MAgnetized Disk and Mirror Axion eXperiment (MADMAX). The experimental setup employs a dielectric haloscope consisting of three sapphire disks and a mirror to resonantly enhance the axion-induced microwave signal within the magnetic dipole field provided by the 1.6 T Morpurgo magnet at CERN. Over 14.5 days of data collection, no axion signal was detected. A 95% CL upper limit on the axion-photon coupling strength down to gaγ2×1011GeV1|g_{a\gamma}| \sim 2 \times 10^{-11} \mathrm{GeV}^{-1} is set in the targeted mass ranges, surpassing previous constraints, assuming a local axion dark matter density ρa\rho_{a} of 0.3 GeV/cm30.3~\mathrm{GeV}/\mathrm{cm}^3. This study marks the first axion dark matter search using a dielectric haloscope.


FIG. 2. Energy density evolution for different initial charges and winding n ¼ 0. The third column shows the integrated charge and energy as functions of time.
FIG. 6. f PBH as a function of M BH . Shaded areas represent existing constraints-we refer the reader to [19,101,102] for an accurate description. The ones on the left follows from Hawking evaporation and are, therefore, only mildly affected by the most conservative estimates of memory burden effect, k ¼ 1 [see (2)]. Dotted lines represent the monochromatic distribution at formation time t f . PBHs lighter than 10 14 g (ignoring corrections due to large number of species) are affected by the burden over cosmological times, resulting in a smearing of the distribution, with spread of order M Ã , for t ≳ t M . The qualitative spread is schematically shown by the red-dashed line.
Memory burden effect in black holes and solitons: Implications for PBH

September 2024

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10 Reads

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15 Citations

Physical Review D

The essence of the memory burden effect is that a load of information carried by a system stabilizes it. This universal effect is especially prominent in systems with a high capacity of information storage, such as black holes and other objects with maximal microstate degeneracy, the entities universally referred to as “saturons.” The phenomenon has several implications. The memory burden effect suppresses a further decay of a black hole, the latest, after it has emitted about half of its initial mass. As a consequence, the light primordial black holes that previously were assumed to be fully evaporated are expected to be present as viable dark matter candidates. In the present paper, we deepen the understanding of the memory burden effect. We first identify various memory burden regimes in generic Hamiltonian systems and then establish a precise correspondence in solitons and in black holes. We make transparent, at a microscopic level, the fundamental differences between the stabilization by a quantum memory burden versus the stabilization by a long-range classical hair due to a spin or an electric charge. We identify certain new features of potential observational interest, such as the model-independent spread of the stabilized masses of initially degenerate primordial black holes. Published by the American Physical Society 2024


Electroweak ηw\eta_w meson

August 2024

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17 Reads

We argue that the Standard Model is accompanied by a new pseudo-scalar degree of freedom, ηw\eta_w-meson, which cancels the topological susceptibility of the electroweak vacuum and gets its mass from this effect. The prediction is based on the analyticity properties of the Chern-Simons correlator combined with the basic features of gravity. Depending on the quality-level of the U(1)B+LU(1)_{B+L}-symmetry, ηw\eta_w emerges as a B+L pseudo-Goldstone boson or as a St\"uckelberg 2-form of the electroweak gauge redundancy. An intriguing scenario of the first category is the emergence of ηw\eta_w in the form of the phase of a U(1)B+LU(1)_{B+L}-violating fermion condensate triggered by the instantons, somewhat similarly to η\eta'-meson in QCD. Regardless of its particular origin, the presence of ηw\eta_w-meson in the theory appears to be a matter of consistency.


New mass window for primordial black holes as dark matter from the memory burden effect

August 2024

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10 Reads

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25 Citations

Physical Review D

The mass ranges allowed for primordial black holes (PBHs) to constitute all of dark matter (DM) are broadly constrained. However, these constraints rely on the standard semiclassical approximation which assumes that the evaporation process is self-similar. Quantum effects such as memory burden take the evaporation process out of the semiclassical regime latest by the time the black hole loses half of its mass. What happens beyond this time is currently not known. However, theoretical evidence based on prototype models indicates that the evaporation slows down, thereby extending the lifetime of a black hole. This modifies the mass ranges constrained, in particular, by big bang nucleosynthesis (BBN) and cosmic microwave background spectral distortions. We show that previous constraints are largely relaxed when the PBH lifetime is extended, making it possible for PBHs to constitute all of DM in previously excluded mass ranges. In particular, this is the case for PBHs lighter than 10 9 g that enter the memory burden stage before BBN and are still present today as DM. Published by the American Physical Society 2024


FIG. 1. Experimental Setup. It is placed in an RF-isolated Faraday cage indicated by the dashed line. To determine the boost factor, a bead can be inserted into the booster to measure the electric field induced by a reflection measurement. Sketch not to scale.
FIG. 1. The MADMAX prototype setup in the shielded laboratory SHELL at DESY/University of Hamburg. The dashed line indicates the path of a putative dark photon signal. The individual components are: 1) Booster consisting of three dielectric disks and a metallic mirror with 30 cm diameter. 2) Focusing mirror. 3) Horn antenna. 4,6,8) Low noise amplifiers. 5,7,9) Bandpass filters. 10) Mixer. 11) Local oscillator. 12) Lowpass filter. 13) DAQ. A Faraday cage and RF absorbers provide additional shielding against external interference.
FIG. 2. Results of the boost factor determination using the bead-pull method. (a) Transverse integrated electric field along the optical axis inside the booster at 19.48 GHz. Measurements (circles) fitted with a model (solid line) including the bead. The dashed line shows the field evaluated without the effect of the bead. The shaded band indicates model uncertainties from material and geometry parameters. The relative difference between fit (F) and measurement (M) is shown in the lower panel. (b) Boost factor as a function of frequency, including the corrections for the finite domain and receiver mismatch. The insets show the transverse electric field between the mirror and the first disk at the indicated frequencies (stars), where grey areas indicate regions unprobed due to mechanical constraints.
FIG. 3. Observed cross-correlated power excess as a function of frequency. The inset shows a zoomed-in view around 19.48 GHz where the maximum boost factor occurs. A hypothetical DP signal with χ = 2 × 10 −13 (magenta solid line) is superimposed on observations (blue circles).
FIG. 3. Booster reflection coefficient Γ as a function of frequency. The booster resonance manifests itself as a broad dip around 19.5 GHz that is superimposed by a standing wave pattern due to reflections between the antenna and booster. The sharp dip at 19.55 GHz is mainly caused by the latter.
First search for dark photon dark matter with a MADMAX prototype

August 2024

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35 Reads

We report the first result from a dark photon dark matter search in the mass range from 78.62{78.62} to 83.95 μeV/c283.95~\mathrm{\mu eV}/c^2 with a dielectric haloscope prototype for MADMAX (Magnetized Disc and Mirror Axion eXperiment). Putative dark photons would convert to observable photons within a stack consisting of three sapphire disks and a mirror. The emitted power of this system is received by an antenna and successively digitized using a low-noise receiver. No dark photon signal has been observed. Assuming unpolarized dark photon dark matter with a local density of ρχ=0.3 GeV/cm3\rho_{\chi}=0.3~\mathrm{GeV/cm^3} we exclude a dark photon to photon mixing parameter χ>3.0×1012\chi > 3.0 \times 10^{-12} over the full mass range and χ>1.2×1013\chi > 1.2 \times 10^{-13} at a mass of 80.57 μeV/c280.57~\mathrm{\mu eV}/c^2 with a 95\% confidence level. This is the first physics result from a MADMAX prototype and exceeds previous constraints on χ\chi in this mass range by up to almost three orders of magnitude.


Citations (58)


... with system temperature T sys , radius r of the disks and mirror, effective data-taking time ∆t, and the local axion DM density ρ a . The Madmax Collaboration has made significant progress in advancing the development of a future largescale dielectric haloscope [26][27][28][29][30][31][32][33]. Small-scale setups have successfully validated the dielectric haloscope approach in dark photon DM searches [34,35], specifically with a broadband Madmax prototype [35]. ...

Reference:

First search for axion dark matter with a Madmax prototype
First mechanical realization of a tunable dielectric haloscope for the MADMAX axion search experiment
  • Citing Article
  • November 2024

Journal of Instrumentation

... In the UV, the phase of the adjoint then plays the role of the (R-) axion. The R-axion has been studied in different contexts [21][22][23][24][25][26][27][28][29][30] including collider phenomenology [31][32][33]. In the lowenergy effective theory there is only 6 an N = 2 gauge multiplet, A, whose scalar component has charge 2 under the IR R-symmetry [19]. ...

Hint to supersymmetry from the GR vacuum

Physical Review D

... However, recent theoretical advancements have challenged this view. The mechanism responsible for extending the PBH lifetime is known as the memory burden effect [38][39][40][41][42][43][44][45][46][47][48], which significantly suppresses the evaporation process and allow these PBHs to persist as DM candidates up to the present day [49][50][51][52][53]. ...

Memory burden effect in black holes and solitons: Implications for PBH

Physical Review D

... However, recent theoretical advancements have challenged this view. The mechanism responsible for extending the PBH lifetime is known as the memory burden effect [38][39][40][41][42][43][44][45][46][47][48], which significantly suppresses the evaporation process and allow these PBHs to persist as DM candidates up to the present day [49][50][51][52][53]. ...

New mass window for primordial black holes as dark matter from the memory burden effect

Physical Review D

... A GWB at high frequencies could potentially be sourced by a collection of exotic physical phenomena originating both in the early and late Universe. Examples include the merging of primordial black holes (PBHs) [18][19][20][21][22][23][24][25] or boson stars [26,27], black hole (BH) superradiance [28], models of modified gravity [29,30], the primordial thermal plasma [31], phase transitions in the early Universe [32][33][34], the "slingshot" mechanism, taking place upon the coexistence of confined and unconfined vacua in the presence of heavy quarks [35], a network of cosmic strings [36][37][38][39][40], post-inflation (p)reheating [41,42], and inflationary mechanisms [43,44]. A novel avenue for detecting GWs at such high frequencies in the GW spectrum has gained momentum in recent years, with various proposal being explored including interferometers [45][46][47][48], microwave and optical cavities [49][50][51][52][53][54], mechanical resonators [55][56][57][58][59][60], superconducting rings [61], and superconducting resonant cavities [62]. ...

Confinement slingshot and gravitational waves

Physical Review D

... Recently, it has been pointed out that the semiclassical description of Hawking evaporation can not hold over the entire black hole lifetime, and one must take into account the effects of quantum backreaction on the black hole over the evaporation timescale. An efficient way to take this backreaction into account is through the so-called "memory burden" effect, which assumes a black hole as a saturated coherent state or a Bose-Einstein condensate bound state of soft gravitons [43][44][45][46]. This suggests that the semiclassical formalism of Hawking -1 - ...

Memory Burden Effect in Black Holes and Solitons: Implications for PBH

... Saturated configurations also appear in nongravitational theories, such as renormalizable field theories [60,62,63]. Saturated configurations not only follow an area law, but also share several properties with BHs, such as thermal-like evaporation [64,65], the presence of an information horizon in the semiclassical regime [60,[62][63][64][65][66], a timescale for information retrieval corresponding to the half-time of evaporation [60,64,65], and a maximal spin bound that cannot exceed their entropy-akin to the extremality condition for spinning BHs [67,68]. This suggests that many features traditionally associated with BHs may arise from the broader behavior of saturated configurations, rather than being unique to gravity. ...

Vortex Effects in Merging Black Holes and Saturons

Physical Review Letters

... The early examples of such effects include the neutron transitions into its hidden copies [43][44][45]. It was shown recently [46] that within the framework of large extra dimensions [47], the "disappearance" or oscillations of a cold neutron into the extra dimensions is a rather generic phenomenon. Moreover, this effect can be linked with the extra-dimensional origin of the neutrino mass [48,49]. ...

Kaluza-Klein spectroscopy from neutron oscillations into hidden dimensions

Physical Review D

... This observation is particularly interesting since "quantum breaking" has provided indications that eternal de Sitter states must not exist in a consistent theory of quantum gravity [93][94][95][96][97][98][99] (see also [100][101][102][103] for similar conjectures in string theory). However, the presence ofθ-vacua in QCD would lead to de Sitter states, and so the only way out is to make theθ-angle unphysical by the addition of an axion -its existence becomes a mandatory consistency requirement, independently of any naturalness considerations [104][105][106]. Our proposal completes the picture as gravity also provides the necessary ALP. ...

The role of gravity in naturalness versus consistency: strong-CP and dark energy