The CDF II measurement of $W$ boson mass is at significant ($6.9\sigma$) tension with the Standard Model, and moderate ($4.0\sigma$) tension with recent results from ATLAS. Any attempt to interpret this as a signature of new physics requires high-precision, robust, falsifiable predictions. The Classical Analogue to the Standard Model In pseudo-Riemannian space–time (CASMIR) is an analogue model predicting $W$ and $Z$ boson masses of $80.3587(22)\mathrm{\text{GeV}}/c^2$ and $91.1877(35)\mathrm{\text{GeV}}/c^2$, respectively. During baryon collisions satisfying $\sqrt{s}<3.09\mathrm{\text{TeV}}$, CASMIR predicts a color-mediated enhancement of $W$ and $Z$ boson masses, becoming $80.4340(22)\mathrm{\text{GeV}}/c^2$ and $91.1922(35)\mathrm{\text{GeV}}/c^2$, respectively. The unenhanced masses are consistent with ATLAS data collected at $\sqrt{s}=7\mathrm{\text{TeV}}$, and the enhanced masses are consistent with CDF II data collected at $\sqrt{s}=1.96\mathrm{\text{TeV}}$. According to CASMIR, operation of the Large Hadron Collider (LHC) at center-of-mass energies small compared with $3.09\mathrm{\text{TeV}}$ but large enough for $W$ boson formation should permit ATLAS to replicate the result from CDF II.

CDF II 测量$瓦$ 玻色子质量显着（$6。9\sigma$) 与标准模型的张力，以及适度的 ($4。0\sigma$）对 ATLAS 的最新结果感到紧张。任何将其解释为新物理学标志的尝试都需要高精度、稳健、可证伪的预测。伪黎曼时空标准模型的经典模拟 (CASMIR) 是一个模拟模型预测$瓦$和$Z$玻色子质量$80。3587（22）\mathrm{\text{GeV}}/C^2$和$91。1877（35）\mathrm{\text{GeV}}/C^2$， 分别。在重子碰撞期间满足$\sqrt{s}<3。09\mathrm{\text{TeV}}$，CASMIR 预测颜色介导的增强$瓦$和$Z$玻色子质量，成为$80。4340（22）\mathrm{\text{GeV}}/C^2$和$91。1922（35）\mathrm{\text{GeV}}/C^2$， 分别。未增强的质量与 ATLAS 收集的数据一致$\sqrt{s}=7\mathrm{\text{TeV}}$，增强的质量与收集的 CDF II 数据一致$\sqrt{s}=1。96\mathrm{\text{TeV}}$。根据 CASMIR 的说法，大型强子对撞机 (LHC) 的质心能量与$3。09\mathrm{\text{TeV}}$但足够大$瓦$玻色子的形成应该允许 ATLAS 复制 CDF II 的结果。