We are concerned with the global structure of positive solutions for p-Laplacian Neumann problem: where \(\varphi _p(s)=\vert s\vert ^{p-2}s\) , \(p>1\) , \(\lambda >0\) is a parameter, \(h:[0,1]\rightarrow \mathbb {R}\) is a continuous function with \(\int _0^1h(x)\text {d}x<0\) , \(g:[0,\infty )\rightarrow [0,\infty )\) is a continuous function satisfying \(\lim _{s\rightarrow 0}g(s)/\varphi _p(s)=0\) and \(\lim _{s\rightarrow \infty }g(s)/\varphi _p(s)=0\) . We obtain a \(\subset \) -shaped component of positive solutions of problem (P) provided suitable conditions. That is, there exist \(\lambda ^*>\lambda _*>0\) , such that the problem (P) has two positive solutions for \(\lambda >\lambda ^*\) and no positive solution for \(\lambda <\lambda _*\) . The proof of main result is based upon bifurcation technology. In addition, to prove the main result, we investigate the principal eigenvalue of auxiliary problem: \(\begin{aligned} \left\{ \begin{array}{l} -(\varphi _p(u'))'+\frac{1}{m}\varphi _p(u)=\lambda h(x) \varphi _p(u),\ \ x\in (0,1),\\ u'(0)=u'(1)=0, \ \ \\ \end{array}\right. \end{aligned}\) where \(m\in \mathbb {N}^+\) .