JS1.2 Increased frequency of paraneoplastic encephalitis with anti-Ma2 antibodies in the cancer immunotherapy era

BACKGROUND

Given the mechanism of action of immune checkpoint inhibitors (ICIs), a possible association with the development of paraneoplastic neurological syndromes (PNS) has been hypothesized. We sought to determine if ICI treatment might trigger anti-Ma2 antibody-associated paraneoplastic neurological syndromes (Ma2-PNS).

MATERIAL AND METHODS

We performed a retrospective nationwide study of all patients with Ma2-PNS developed during ICI treatment between 2017–2018. The frequency of neuronal-antibody detection before and after ICI implementation was also analyzed.

RESULTS

Our series of patients included 5 men and 1 woman (median age, 63 years). The patients were receiving either nivolumab (n = 3), pembrolizumab (n = 2) or a combination of nivolumab and ipilimumab (n=1), for treatment of neoplasms that included lung (n=4) and kidney (n=1) cancers, and pleural mesothelioma (n=1). Median delay between ICI introduction and onset of the neurological syndrome was 4 months. Clinical syndromes included a combination of limbic encephalitis and diencephalitis (n=3), isolated limbic encephalitis (n=2) and a syndrome characterized by opthalmoplegia and head-drop (n=1). Patients with diencephalitis manifested hyperphagia, weight gain and somnolence. Post-ICI Ma2-PNS accounted for 35% of the total 17 Ma2-PNS diagnosed in our center over the 2017–2018 biennium. Eight cases had been detected in the preceding biennium 2015–2016, corresponding to a 112% increase of Ma2-PNS frequency since the implementation of ICIs in France. No other neuronal-antibody demonstrated a similar increment.

CONCLUSION

We show a clear association between ICI use and increased frequency of Ma2-PNS. Physicians need to be aware that ICIs can trigger Ma2-PNS since clinical presentation can be challenging.

A comparison of "flat fielding" techniques for x-ray framing cameras

Gain can vary across the active area of an x-ray framing camera by a factor of 4 (or more!) due to the voltage loss and dispersion associated with pulse transmission in a microstripline-coated microchannel plate. In order to make quantitative measurements, it is consequently important to measure the gain variation ("flat field"). Moreover, because of electromagnetic cross talk, gain variation depends on specific operational parameters, and ideally a flat field would be obtained at all operating conditions. As part of a collaboration between Lawrence Livermore National Laboratory's National Ignition Facility and the Commissariat à l'Énergie Atomique, we have been able to evaluate the consistency of three different methods of measuring x-ray flat fields. By applying all three methods to a single camera, we are able to isolate performance from method. Here we report the consistency of the methods and discuss systematic issues with the implementation and analysis of each.

Picosecond X-ray streak camera dynamic range measurement

Streak cameras are widely used to record the spatio-temporal evolution of laser-induced plasma. A prototype of picosecond X-ray streak camera has been developed and tested by Commissariat à l'Énergie Atomique et aux Énergies Alternatives to answer the Laser MegaJoule specific needs. The dynamic range of this instrument is measured with picosecond X-ray pulses generated by the interaction of a laser beam and a copper target. The required value of 100 is reached only in the configurations combining the slowest sweeping speed and optimization of the streak tube electron throughput by an appropriate choice of high voltages applied to its electrodes.

First set of gated x-ray imaging diagnostics for the Laser Megajoule facility

The Laser Megajoule (LMJ) facility located at CEA/CESTA started to operate in the early 2014 with two quadruplets (20 kJ at 351 nm) focused on target for the first experimental campaign. We present here the first set of gated x-ray imaging (GXI) diagnostics implemented on LMJ since mid-2014. This set consists of two imaging diagnostics with spatial, temporal, and broadband spectral resolution. These diagnostics will give basic measurements, during the entire life of the facility, such as position, structure, and balance of beams, but they will also be used to characterize gas filled target implosion symmetry and timing, to study x-ray radiography and hydrodynamic instabilities. The design requires a vulnerability approach, because components will operate in a harsh environment induced by neutron fluxes, gamma rays, debris, and shrapnel. Grazing incidence x-ray microscopes are fielded as far as possible away from the target to minimize potential damage and signal noise due to these sources. These imaging diagnostics incorporate microscopes with large source-to-optic distance and large size gated microchannel plate detectors. Microscopes include optics with grazing incidence mirrors, pinholes, and refractive lenses. Spatial, temporal, and spectral performances have been measured on x-ray tubes and UV lasers at CEA-DIF and at Physikalisch-Technische Bundesanstalt BESSY II synchrotron prior to be set on LMJ. GXI-1 and GXI-2 designs, metrology, and first experiments on LMJ are presented here.

Overview of the ARGOS X-ray framing camera for Laser MegaJoule

Commissariat à l'Énergie Atomique et aux Énergies Alternatives has developed the ARGOS X-ray framing camera to perform two-dimensional, high-timing resolution imaging of an imploding target on the French high-power laser facility Laser MegaJoule. The main features of this camera are: a microchannel plate gated X-ray detector, a spring-loaded CCD camera that maintains proximity focus in any orientation, and electronics packages that provide remotely-selectable high-voltages to modify the exposure-time of the camera. These components are integrated into an "air-box" that protects them from the harsh environmental conditions. A miniaturized X-ray generator is also part of the device for in situ self-testing purposes.

Diagnostics hardening for harsh environment in Laser Megajoule (invited)

The diagnostic designs for the Laser Megajoule (LMJ) will require components to operate in environments far more severe than those encountered in present facilities. This harsh environment will be induced by fluxes of neutrons, gamma rays, energetic ions, electromagnetic radiations, and, in some cases, debris and shrapnel, at levels several orders of magnitude higher than those experienced today on existing facilities. The lessons learned about the vulnerabilities of present diagnostic parts fielded mainly on OMEGA for many years, have been very useful guide for the design of future LMJ diagnostics. The present and future LMJ diagnostic designs including this vulnerability approach and their main mitigation techniques will be presented together with the main characteristics of the LMJ facility that provide for diagnostic protection.