The phrase "Due to Lorentz invariance, only the Higgs particle can have a non-zero expected value in a vacuum" refers to the unique properties of scalar fields, specifically the Higgs field. The vacuum expectation value (VEV) is a characteristic of the Higgs field, not the Higgs boson itself, as there are no Higgs bosons present in a vacuum. Non-scalar fields would disrupt Lorentz invariance by introducing a preferred direction, which is not the case with scalar fields. While tensor fields can have non-vanishing VEVs, they are not part of the Standard Model, reinforcing the special status of scalar fields. The statement is mathematically supported, emphasizing that only scalar fields can maintain Poincare symmetry with non-zero VEVs.