To begin my blog, let’s introduce parahydrogen. Lately, this little molecule has been attracting a lot of attention in the magnetic resonance community due to tremendous opportunities it brings for NMR/MRI signal enhancement. I will explain a bit later how this parahydrogen-based NMR signal enhancement works. But first, let’s talk about physical origins of parahydrogen!

Parahydrogen (*para*-H_{2}) is a nuclear spin isomer of a hydrogen molecule. Nuclear spin isomerism is a very special form of isomerism. Unlike “traditional” molecular isomers (molecules having the same atomic composition but different chemical structure) and isotopologues (isomers that differ only in their isotopic composition), nuclear spin isomers are chemically identical: they have exactly the same atomic (and even isotopic) structure. However, nuclear spin isomers differ in the nuclear spin state of their atoms. It turns out that this tiny change (energy difference associated with nuclear spin transitions is only ~0.1 J/mol) may lead to different thermodynamic and spectroscopic properties of molecules. So, how does this work?

Unfortunately (or fortunately), we will have to use rules of quantum mechanics and some math. In quantum mechanics, in order to describe properties of quantum systems (atoms, molecules, *etc*.), physicists use wavefunctions. By knowing a wavefunction one will be able to calculate probabilities to find a quantum system in different states (namely, a squared modulus of the wavefunction determines the probability to find a system in a given state). Let’s look how it works taking as an example hydrogen molecule.

Hydrogen molecule consists of two hydrogen atoms (H) and is denoted as Н_{2}. Each atom has a nucleus – a proton which is a spin-1/2 particle. Physicists say that hydrogen molecule has several degrees of freedom: translational, rotational, vibrational, *etc*., and these degrees of freedom can be considered independent. In other words, rotation of the hydrogen molecule does not depend on how and where the molecule is moving and how it is vibrating. Each degree of freedom has a wavefunction associated with it. I will use different colors to describe electron and nuclear wavefunctions. A position of the molecule in space, as well as its rotation and vibrations, are determined by the position and movements of nuclei, therefore, these degrees of freedom are described by translational (*ψ*_{tr}), rotational (*ψ*_{rot}), vibrational (*ψ*_{vib}), and nuclear spin (*ψ*_{spin}) wavefunctions. Atomic nuclei are surrounded by electrons which provides the bonding between the nuclei. The wavefunction describing movements of electrons is called orbital wavefunction *ψ*_{orb}, and state of the electron spins is described by the electron spin wavefunction *ψ*_{spin}.

Since probabilities of independent events are multiplied, the total wavefunction is a product of the above-mentioned wavefunctions:

** ψ_{tot}** =

*ψ*

_{tr}

*·*

*ψ*

_{rot}

*·ψ*

_{vib}

*·ψ*

_{spin}

*·ψ*

_{orb}

*·ψ*

_{spin}

However, rules of quantum mechanics are trickier than they may sound. According to Pauli’s principle, the total wavefunction of the system of spins-1/2 particles has to be antisymmetric with respect to the exchange (also called permutation) of two identical particles. What does this mean?

Let’s take for example *ψ*_{spin}. A system consisting of two spins-1/2 can be described as *α*^{1}*α*^{2}, *β*^{1}*β*^{2} or combinations *α*^{1}*β*^{2}+*β*^{1}*α*^{2}, *α*^{1}*β*^{2}–*β*^{1}*α*^{2}. Here *α* and *β* denote the projection of nuclear spin angular momentum along the quantization axis (more on this stuff later, for now, one can imagine the state *α* as a magnetic moment – spin – pointing up along the external magnetic field and the state *β *as a magnetic moment pointing down, opposite to the field). Indexes 1 and 2 say to which nucleus the spin belongs. For example, the state *α*^{1}*α*^{2} means that both nuclear spins point along the field while the state *β*^{1}*β*^{2} means that both spins point opposite to the field. The combination states *α*^{1}*β*^{2}+*β*^{1}*α*^{2} and *α*^{1}*β*^{2}–*β*^{1}*α*^{2} are more interesting. Neither of spins points along or opposite to the field but if we take one spin and determine its orientation, the second spin will take the opposite orientation. We can see now that two spins are correlated: the state of the second spin depends on the state of the first one.

Now let’s look what happens if we exchange (permute) particles. Mathematically, permutation simply means interchange of indexes (1→2, 2→1). One can see that upon permutation of indexes the first three states do not change: *α*^{2}*α*^{1}= *α*^{1}*α*^{2}, *β*^{2}*β*^{1} = *β*^{1}*β*^{2}, *(**α*^{2}*β*^{1}+*β*^{2}*α ^{1}) = (*

*α*

^{1}

*β*

^{2}+

*β*

^{1}

*α*

^{2}

*)*, but the last state changes the sign:

*(*

*α*

^{2}

*β*

^{1}–

*β*

^{2}

*α*

^{1}) = –(*α*

^{1}

*β*

^{2}–

*β*

^{1}

*α*

^{2}

*)*. Therefore, the first three states are called

*symmetric*wavefunctions and the last one –

*antisymmetric*with respect to permutation of particles.

So, our hydrogen molecule contains four spin-1/2 particles: two electrons and two nuclei). Permutation of electrons can only affect *ψ*_{orb}* *and* ψ*_{spin}. The first wave function, corresponding to the electronic ground state, is symmetric with respect to the electrons, the second, the electron spin wavefunction, is antisymmetric, and the rest are independent of the electrons’ variables and, thus, symmetric. Therefore, Pauli’s principle is fulfilled for electrons: the total wavefunction is antisymmetric with respect to permutation of electrons, thanks to antisymmetric *ψ*_{spin}. Permutation of nuclei can affect two wavefunctions: *ψ*_{spin} (as we just saw above) and *ψ*_{rot}. A mathematical expression for *ψ*_{rot} is rather complicated but it is not necessary to know its full form to understand the symmetry properties.

This is because rotating diatomic molecules possess a set of stable rotational states, which can be described by only one parameter – the rotational quantum number *J*. This number can take integer values 0, 1, 2, 3, … This means that molecule can be in a stable state with *J* = 0, *J* = 1, *J* = 2, *etc*. (**Figure 1**). It turns out that the symmetry (with respect to permutation of nuclei) of the rotational wavefunction can be described as

*P*_{12}*·ψ*_{rot} = (-1)^{J}*·ψ*_{rot}

where *P*_{12} represents the permutation operator that interchanges the nuclei’s positions (indexes). This means that the rotational wavefunction is symmetric for even rotational states (*J* = 0, 2, 4, …) and antisymmetric for odd rotational states (*J = *1, 3, 5, …).

Coming back to Pauli’s principle, permutation of nuclei should lead to the change of sign of the total wavefunction. Since only *ψ*_{spin} and *ψ*_{rot} can change sign upon such permutation, these two wavefunctions become connected: even (symmetric) rotational wavefunctions must be combined with the antisymmetric nuclear wavefunction *(**α*^{1}*β*^{2}–*β*^{1}*α*^{2}*)*, whereas each antisymmetric rotational wavefunction has to be associated with one of the three symmetric spin functions. All this is required to yield a total wavefunction being antisymmetric with respect to the exchange of the nuclei. This is where two hydrogen spin isomers come from. One is called parahydrogen (*para*-H_{2}), having an antisymmetric nuclear spin wavefunction *(α*^{1}*β*^{2}–*β*^{1}*α*^{2}*)* and existing only in even rotational states, and the other called orthohydrogen (*ortho*-H_{2}), having a symmetric nuclear spin wavefunction and existing only in the odd rotational states.

It follows from the Pauli’s principle that nuclear spin state and rotational state of the hydrogen molecule are strictly correlated. This is remarkable, because the notion of independence (which allowed us to write a wavefunction as a product of individual wavefunctions) has led to complete dependence of these degrees of freedom from each other!

Remarkably, parahydrogen and orthohydrogen can be seen as two individual gases because their thermodynamic properties (boiling point, heat capacity, *etc*.) are slightly different. This is not surprising taking into account the fact that molecules constituting these two gases are rotating differently!

Importantly, conversion between the two states occurs extremely slowly because the transition between symmetric and antisymmetric nuclear spin states are forbidden by the selection rules of quantum mechanics. Therefore, after its production parahydrogen may be stored for long periods before use in a tank as an individual gas, as the relaxation rate of the parahydrogen back to room-temperature equilibrium can be on the order of months.

However, the use of paramagnetic catalysts (*i.e.*, activated charcoal, nickel, hydrated iron(III) oxide) promotes the establishment of Boltzmann thermodynamic equilibrium between *ortho*-H_{2}/*para*-H_{2} states for a given temperature at greatly accelerated rates. This happens because paramagnetic materials can create a strong inhomogeneous magnetic field on the atomic scale. In such fields the two hydrogen atoms are no longer equivalent, thus, spin-flip transitions between *ortho*-H_{2} and *para*-H_{2} are no longer forbidden. In practice, normal hydrogen gas (*i.e.*, equilibrium ratio of spin isomers at room temperature) consisting of 75% *ortho*– and 25% *para*-hydrogen is passed through a chamber filled with paramagnetic catalyst and maintained at cryogenic temperatures, where the equilibration to the isomer ratio governed by the Boltzmann distribution occurs. For example, a parahydrogen generator operating at 77 K (obtained conveniently by a liquid-N_{2} bath) yields a mixture with ~50% parahydrogen, whereas the designs based on cryo-chillers (*e.g.* T~20 K) yield >99% parahydrogen (**Figure 2**). I should note that the enrichment of hydrogen with *para*-isomer happens so easily only because of the big energy gap between rotational spin states. This, in turn, is due to the small mass of molecular hydrogen (in general, the energy difference between rotational spin states is inversely proportional to the moment of inertia of a rotating molecule).

The existence of nuclear spin isomers of molecular hydrogen (which was experimentally confirmed by the early 1930s) was one of the first triumphs of quantum mechanics. Indeed, the citation of the Nobel Prize awarded to Werner Heisenberg in 1932 stated that he had “created quantum mechanics, the application of which led to the discovery of the two allotropic forms of hydrogen”!

Knowledge about *ortho*– to *para*-H_{2} conversion is important for the storage of liquid hydrogen (especially as a rocket fuel). The difference in energy associated with the different rotational levels means that energy is released when *ortho*-H_{2} converts to *para*-H_{2}, and energy is absorbed in the reverse process. This phenomenon can be thought of as a latent heat of conversion. If one quickly liquefies normal hydrogen, it will still have 3:1 *ortho*:*para* composition which will eventually lead to the heat release. This can vaporize a significant portion of hydrogen and break the impermeability of the storage container. At the dawn of industrial liquid hydrogen production, this presented a major problem. Modern hydrogen liquefying processes now ensure that the liquid hydrogen has reached equilibrium concentration at 99.8% *para*-H_{2} before being transported and stored for use.

One may ask how can *para*-H_{2} be important for NMR? Indeed, this spin isomer has a zero total nuclear spin and, thus, it does not possess ^{1}H NMR spectrum. However, *para*-H_{2} is a pure quantum mechanical state and a highly organized spin order which is readily achievable simply by cooling. Pure state means that all *para*-H_{2} molecules are described by the same wavefunction – *(α*^{1}*β*^{2}–*β*^{1}*α*^{2}*). *For comparison, *ortho*-H_{2} is a mixture of three wavefunctions, *α*^{1}*α*^{2}, *α*^{1}*β*^{2}+*β*^{1}*α*^{2} and *β*^{1}*β*^{2} and, thus, it is not a pure state. It turns out that once you have a quantum mechanically pure state, you can manipulate it and transfer the spin order from one form to another. This is how parahydrogen-induced polarization (PHIP) and signal amplification by reversible exchange (SABRE) work: they transfer NMR-silent singlet spin order of *para*-H_{2} into observable nuclear magnetization.

[…] let’s talk about physical principles of this effect. As we discussed before, due to the absence of a net nuclear magnetic moment, para-H2 itself does not produce an NMR […]

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