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The following is a summary of “Emerging therapeutic frontiers in cancer: insights into posttranslational modifications of PD-1/PD-L1 and regulatory pathways,” published in the April 2024 issue of Hematology by Wang et al.

The intricate interplay between programmed cell death ligand 1 (PD-L1), expressed on the surface of tumor cells, and programmed cell death 1 (PD-1), expressed on T cells, constitutes a pivotal mechanism fostering immune evasion by tumor cells through the thwarting of effective tumor antigen-specific T cell activation. The advent of PD-1/PD-L1 blockade has emerged as a transformative strategy in combating tumor immune evasion, garnering substantial interest within the oncology landscape. Clinical investigations have underscored the remarkable efficacy and safety profile of PD-1/PD-L1 blocking antibodies across a spectrum of malignancies, offering a beacon of hope for patients.

Nonetheless, the therapeutic landscape of anti-PD-1/PD-L1 interventions is fraught with challenges, including limited indications and the emergence of drug resistance, necessitating a nuanced approach to therapeutic intervention. Accordingly, unraveling additional regulatory pathways and molecular players associated with PD-1/PD-L1 signaling assumes paramount importance, alongside the strategic implementation of combinational therapeutic modalities, to address the multifaceted dynamics of tumor immune evasion.

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A research team led by the late Professor Liang Haojun from the Hefei National Laboratory for Physical Sciences at the Microscale of University of Science and Technology of China (USTC) has developed a facile enthalpy-mediated strategy to precisely control the replication and catalytic assembly of DNA-functionalized colloids in a time-dependent manner, facilitating the creation of large-scale ordered nanomaterials. The study was published in Angewandte Chemie International Edition.

The replication of information is a fundamental characteristic of nature, with playing a crucial role in . However, creating synthetic systems that can produce large-scale, three-dimensionally ordered nanomaterials using self-replicating nanostructures has remained a formidable challenge.

Existing artificial self-replicating systems often fall short in programmable assembly into sophisticated nanostructures, limiting their potential functions and applications.

The elegant equations of classical electromagnetism written by James Clark Maxwell in 1861 display a remarkable symmetry between electric and magnetic fields except for their sources. We know about electric charges but we have not found magnetic charges. Bar magnets are dipoles with two poles, north and south, for the magnetic field, resembling the configuration of an electric field sourced by a pair of positive and negative electric charges. However, we had never seen experimental evidence for a magnetic monopole, namely a magnetic charge with only one magnetic pole, a net north or south, from where magnetic field lines emanate, just like the electric field sourced by an electric charge. In a symmetric theory of electromagnetism, magnetic monopoles should exist.

The existence of monopoles with a net magnetic charge was proposed by Paul Dirac in 1931 to explain the quantized (discrete) values of electric charges. Dirac found that magnetic charges should be an integer multiple of a fundamental unit, g_D, equal to the electron charge, e, divided by twice the fine-structure constant, or about 68.5e.

In classical physics, the existence of magnetic monopoles restores symmetry to Maxwell’s equations. But in the broader context of quantum mechanics, Gerard ‘t Hooft and Alexander Polyakov showed in 1974 that magnetic monopoles are required in Grand Unified Theories of the strong, weak and electromagnetic interactions. Since the electric charge is quantized, magnetic charges are unavoidable in these theories. Magnetic charges with the lowest mass must be stable because magnetic charge is conserved and they cannot decay into lower-mass particles.