Quantum Number (QN) Objects
As shown in examples on the previous pages, subspaces of
a QN Index are labeled by QN objects, such as QN("Sz",1)
or QN({"N",2},{"Sz",0}). This page goes into more detail
about how these QN objects work, what mathematical rules
they obey, and how to construct them.
From a physics perspective, quantum numbers are quantities which are conserved under the dynamics of a system. Examples include total particle number, particle number modulo 2, or total z-axis magnetization. Mathematically, quantum numbers arise from the representation theory of Abelian groups, which relates their irreducible representations to products of @@\mathbb{Z}@@ or @@\mathbb{Z}_n@@ .
QN Object Basics
At the simplest level, a QN is a small set of quantum numbers stored as name-value pairs, where the name is a short string of up to seven characters and the value is an integer.
For example, a QN constructed as QN("N",2) contains one quantum number
named "N" with the value 2.
A QN constructed as QN({"Nb",1},{"Sz",2}) contains two quantum numbers:
one named "Nb" with the value 1, the other named "Sz" of value 2.
QN objects can be added, subtracted, and compared to each other. For QNs like those above, addition and subtraction follows the usual rules of integer arithmetic. Quantum numbers with the same name are added to each other. If a QN contains a quantum number which is not present in another QN, such a case is treated as if the other QN did have that quantum number but with the value equal to zero. This rule about missing quantum numbers being treated as zero applies to addition, subtraction, and comparison.
For example: QN({"N",3}) + QN({"Sz",2},{"N",1}) == QN({"Sz",2},{"N",4}).
As another example, QN({"N",3}) == QN({"Sz",0},{"N",3}) compares true.
The quantum numbers within a QN are not ordered, from a user perspective. Internally they are sorted by name, but you may provide them in any order and the QN system will handle the sorting for you.
Besides regular integer arithmetic, arithmetic modulo N (according to the group @@Z_N@@ ) can also be defined for QN—we will discuss this case more below.
Special Cases of the QN Constructor
Note that when constructing a QN containing just one quantum number,
it is allowed to omit the curly braces: QN("Sz",2).
Also, at most one of the quantum numbers in a QN can be unnamed, which is equivalent
to letting the name be the empty string "". This is for convenience
when no name is obvious. For example, QN(0) and QN(1) are
valid QNs and equivalent to QN({"",0}) and QN({"",1}).
Modular Arithmetic
An important case of quantum numbers for physics applications are quantum numbers obeying a @@Z_N@@ addition rule. Key examples include fermion parity obeying a @@Z_2@@ addition rule or clock-spin models obeying a @@Z_3@@ addition rule.
To specify @@Z_N@@ addition for one or more quantum numbers within a QN,
simply specify the modulus @@N@@ as a third entry when defining that quantum number.
For example, QN("P",0,2) and QN("P",1,2) defines a quantum number named "P"
(for parity) which obeys a @@Z_2@@ addition rule, and which takes the values 0 and
1 in the respective QNs constructed.
Thus QN("P",1,2)+QN("P",1,2) == QN("P",0,2).
Another example would be QN({"Sz",1},{"T",2,3}) which defines a quantum number named
"Sz" with value 1 obeying usual integer arithmetic, whereas the quantum number named
"T" has value 2 and obeys a @@Z_3@@ addition rule.
Advanced / Experimental Features
Currently we are exploring a feature which would allow QN Indices to anticommute to give QN ITensors fermionic behavior, without requiring users to do any bookkeeping such as with Jordan-Wigner string. We are reserving negative QN modulus values for this purpose. Therefore please only set the modulus of a quantum number to a positive number, unless you want automatic fermion feature to be enabled. Right now, AutoMPO uses a subset of these features. If you have any questions, please contact us at [email protected] or post a question on the Support Forum.
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