Is there any self-adjoint operator bounded in all Hilbert spaces with a physical significance in quantum mechanics? 
"To each real-valued function $f$ on the classical phase space, there is associated a self-adjoint operator $\hat{f}$ on the quantum Hilbert space. In almost all cases $\hat{f}$ is unbounded." As an example, position and momentum operators are unbounded in general. They are bounded provided a number of suitable conditions are imposed on the underlined Hilbert space. Identity operator is bounded in all Hilbert space. We have examples of self-adjoint operators, bounded on all Hilbert spaces, which may not have any physical significance. 

My question is if there is a self-adjoint operator other than the identity operator with a physical importance that is bounded on every Hilbert space. If they exist, please provide some examples. If they do not exist, please justify their non-existence.
 A: An operator is, by definition, a linear map from some given linear space $V$ to itself. And the definition of a linear map cannot, in general, be independent of the linear structure if the space it acts upon.
There are, however, algebraic objects that can be defined abstractly, and that they are always represented as bounded operators on some (actually many) Hilbert space(s). These algebraic objects are the ones forming involutive algebras, in particular C*-algebras. It is standard to consider the set of observables of a given physical system as forming an involutive algebra.
In non-relativstic quantum mechanics, the C* algebra of interest is fixed (up to *-isomorphisms), and it is uniquely (up to unitary isomorphisms) irreducibly represented in a Hilbert space. This irreducible representation is the so-called Schrödinger representation on $L^2(\mathbb{R}^d)$, where position and momentum are respectively the self-adjoint unbounded operators of multiplication and $1/i$-times differentiation with respect to the variable $x\in\mathbb{R}^d$. It is in this representation that the pseudodifferential calculus, that associates to (almost) any function (actually distribution) on the phase space $\mathrm{T}^*\mathbb{R}^d$ an operator from $\mathscr{S}(\mathbb{R}^d)$ to $\mathscr{S}'(\mathbb{R}^d)$ (that can, in some case, be restricted to a densely defined operator on $L^2(\mathbb{R}^d)$), is set.
Clarified all that, there are plenty of examples of physically relevant bounded self-adjoint operators in quantum mechanical systems. The foremost example is the spectral family $(P_\lambda)_{\lambda\in \mathbb{R}}$ of a given self-adjoint (possibly unbounded) observable $A$. Many people consider the spectral resolution much more physically relevant than the observable itself (there is a $1-1$ correspondence anyways), for $\lVert (P_{\lambda_1}-P_{\lambda_2})\psi\rVert^2$ is the probability that a measurement of the observable $A$ in the system in the state $\psi$ would yield a value in the interval $[\lambda_2,\lambda_1]\subseteq \mathbb{R}$ (assuming $\lambda_2 < \lambda_1$). The spectral family consists entirely of bounded (self-adjoint) operators (orthogonal projections, that each satisfy $P^2_{\lambda}=P_\lambda$).
A: What about the operator for the energy of a particle in a box? It's easy to see that it is bounded below. It corresponds to discrete sinusoid wave functions with half a wavelength. Different half-wavelength functions differ a little in energy (the ones with the highest energy are the ones with are perpendicular to two opposite walls.
The wavefunctions have un upper limit in the sense that they can't have wavelengths which correspond to energies higher than the energy necessary to make virtual particle pairs real. Well, these wave functions do of course exist, but then we're talking about a different situation than that of a single particle in a box.
It doesn't really matter what Hibert space you choose because the base functions for every space make up the same Hilbert space [like you can find an infinite number of three orthogonal (or non-orthogonal) three-vectors that span three-dimensional space], and the wavefunctions stay the same but expressed in different base functions.
