Let f and g be two Hecke–Maass cusp forms of weight zero for SL2(Z)\documentclass[12pt]{minimal}
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\begin{document}$$SL_2({\mathbb {Z}})$$\end{document} with Laplacian eigenvalues 14+u2\documentclass[12pt]{minimal}
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\begin{document}$$\frac{1}{4}+u^2$$\end{document} and 14+v2\documentclass[12pt]{minimal}
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\begin{document}$$\frac{1}{4}+v^2$$\end{document}, respectively. Then both have real Fourier coefficients say, λf(n)\documentclass[12pt]{minimal}
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\begin{document}$$\lambda _f(n)$$\end{document} and λg(n)\documentclass[12pt]{minimal}
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\begin{document}$$\lambda _g(n)$$\end{document}, and we may normalize f and g so that λf(1)=1=λg(1)\documentclass[12pt]{minimal}
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\begin{document}$$\lambda _f(1)=1=\lambda _g(1)$$\end{document}. In this article, we first prove that the sequence {λf(n)λg(n)}n∈N\documentclass[12pt]{minimal}
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\begin{document}$$\{\lambda _f(n)\lambda _g(n)\}_{n \in {\mathbb {N}}}$$\end{document} has infinitely many sign changes. Then we derive a bound for the first negative coefficient for the same sequence in terms of the Laplacian eigenvalues of f and g.