Maximizing $\sin \beta \cos \beta + \sin \alpha \cos \alpha - \sin \alpha \sin \beta$

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I need to maximize

$$ \sin \beta \cos \beta + \sin \alpha \cos \alpha - \sin \alpha \sin \beta \tag{1}$$

where $\alpha, \beta \in [0, \frac{\pi}{2}]$.

With numerical methods I have found that

$$ \sin \beta \cos \beta + \sin \alpha \cos \alpha - \sin \alpha \sin \beta \leq 2 \sin \frac{\alpha + \beta}{2} \cos \frac{\alpha + \beta}{2} - \sin^2 \frac{\alpha + \beta}{2}. \tag{2} $$

If $(2)$ is true then I can denote $x = \frac{\alpha + \beta}{2}$ and prove (using Cauchy inequality) that

$$ 2 \sin x \cos x - \sin^2 x \leq \frac{\sqrt{5}-1}{2}. \tag{3}$$

But is $(2)$ true? How do I prove it? Maybe I need to use a different idea to maximize $(1)$?

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A nice solution with elementary methods was provided by user arqady in AoPS (see here). It is as follows:

It is easy to see, using the trigonometric addition formulas that

$$ \sin \beta \cos \beta + \sin \alpha \cos \alpha - \sin \alpha \sin \beta=\sin(\alpha+\beta)\cos(\alpha-\beta)-\frac{1}{2}\cos(\alpha-\beta)+\frac{1}{2}\cos(\alpha+\beta) $$

Using Cauchy's inequality,

$$ \sin(\alpha+\beta)\cos(\alpha-\beta)-\frac{1}{2}\cos(\alpha-\beta)+\frac{1}{2}\cos(\alpha+\beta) \leq \sqrt{\cos(\alpha - \beta)^2+\frac{1}{4}}-\frac{1}{2} \cos (\alpha - \beta) $$

and, denoting $\cos(\alpha - \beta) = x$

$$ \sqrt{x^2+\frac{1}{4}}-\frac{1}{2} x \leq\frac{\sqrt5-1}{2} $$

because, after squaring,

$$3x^2 +2x - 2\sqrt{5}x + 2\sqrt{5} - 5 \leq 0 \\ (x-1)(3x+5-2\sqrt{5}) \leq 0$$

which holds because $\alpha, \beta \in [0, \frac{\pi}{2}]$ so $x \in [0, 1]$. (The first term is nonnegative, the second one is positive.)

Equality holds if $\frac{\sin(\alpha + \beta)}{\cos(\alpha - \beta)} = \frac{\cos(\alpha + \beta)}{\frac{1}{2}}$ and $x = 1$. Therefore $\alpha = \beta$ and $\tan 2\alpha = 2$ so

$$ \sin \beta \cos \beta + \sin \alpha \cos \alpha - \sin \alpha \sin \beta \leq \frac{\sqrt5-1}{2}$$

with equality at $\alpha = \beta = \frac{1}{2} \arctan 2$.

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As Dan suggested, solve for the stationary points of the gradient. You'll end up solving two (identical) quartics in $\sin \alpha$, $\sin \beta$ (which are really just 2 quadratics due to the symmetry) and find that the only stationary point in the range is at $\alpha = \beta = \pi/6$. For this to not be the maximum on the domain, the max must occur on the boundary, which are much simpler sub-problems to solve (and by the symmetry you only have to solve 2), and in fact will prove that $\alpha = \beta = \pi/6$ gives the max over the domain.

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Let $$f = \sin \alpha \cos \alpha + \sin \beta \cos \beta -\sin \alpha \sin \beta = \frac{1}{2}(\sin 2\alpha + \sin 2\beta) -\sin \alpha \sin \beta$$

$$\frac{\partial f}{\partial \alpha} = 0 \implies \cos 2\alpha - \sin \beta \cos \alpha = 0$$ $$\frac{\partial f}{\partial \beta} = 0 \implies \cos 2\beta - \sin \alpha \cos \beta = 0$$

From symmetry (also may not be difficult to show directly) $$\beta = \alpha$$

Finally, $$\alpha = \beta = \frac{1}{2} \tan^{-1} 2$$

Substituting in $f$, the maximum value is 0.61803398874989484820