Chosen Fixed Point
Here is the data for the chosen fixed point.
$F_{UV}$ represents the flavor symmetries in the UV Lagrangian, and $F_{IR}$ represents the flavor symmetries in the IR. $F_{UV}$ and $F_{IR}$ can differ due to accidental symmetry enhancement.
The number of marginal operators, $n_{marginal}$, minus the dimension of flavor symmetries in IR, $|F_{IR}|$, corresponds to the coefficient of $t^6$ in the superconformal index.
# | Theory | Superpotential | Central charge $a$ | Central charge $c$ | Ratio $a/c$ | Matter field: $R$-charge | U(1) part of $F_{UV}$ | Rank of $F_{UV}$ | Rational |
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50989 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}q_{1}\tilde{q}_{1}$ + ${ }M_{3}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{3}M_{4}$ + ${ }\phi_{1}^{2}q_{2}\tilde{q}_{1}$ + ${ }M_{5}\phi_{1}^{2}$ + ${ }\phi_{1}q_{1}\tilde{q}_{1}$ + ${ }M_{2}X_{1}$ + ${ }M_{1}^{2}$ | 0.5499 | 0.6749 | 0.8148 | [X:[1.5714], M:[1.0, 0.4286, 0.7143, 1.2857, 1.1429], q:[0.7143, 0.2857], qb:[0.8571, 0.4286], phi:[0.4286]] | [X:[[0]], M:[[0], [0], [0], [0], [0]], q:[[0], [0]], qb:[[0], [0]], phi:[[0]]] | 0 | {a: 1509/2744, c: 463/686, X1: 11/7, M1: 1, M2: 3/7, M3: 5/7, M4: 9/7, M5: 8/7, q1: 5/7, q2: 2/7, qb1: 6/7, qb2: 3/7, phi1: 3/7} |
Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
---|---|---|---|---|
${}M_{3}$, ${ }M_{1}$, ${ }\phi_{1}q_{2}^{2}$, ${ }M_{5}$, ${ }q_{2}\tilde{q}_{1}$, ${ }q_{1}\tilde{q}_{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }M_{4}$, ${ }\phi_{1}\tilde{q}_{2}^{2}$, ${ }M_{3}^{2}$, ${ }\phi_{1}q_{1}q_{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}q_{1}\tilde{q}_{2}$, ${ }X_{1}$, ${ }M_{1}M_{3}$, ${ }M_{3}\phi_{1}q_{2}^{2}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{3}M_{5}$, ${ }\phi_{1}q_{1}^{2}$, ${ }M_{3}q_{1}\tilde{q}_{2}$, ${ }M_{3}\phi_{1}q_{2}\tilde{q}_{2}$ | ${}\phi_{1}^{2}q_{2}^{4}$, ${ }M_{3}\phi_{1}\tilde{q}_{2}^{2}$ | 0 | t^2.143 + 2*t^3. + 4*t^3.429 + 2*t^3.857 + t^4.286 + t^4.714 + 2*t^5.143 + 2*t^5.571 + 5*t^6.429 + 8*t^6.857 + 4*t^7.286 + 3*t^7.714 + 2*t^8.571 - t^4.286/y + (2*t^8.143)/y + (4*t^8.571)/y - t^4.286*y + 2*t^8.143*y + 4*t^8.571*y | t^2.143 + 2*t^3. + 4*t^3.429 + 2*t^3.857 + t^4.286 + t^4.714 + 2*t^5.143 + 2*t^5.571 + 5*t^6.429 + 8*t^6.857 + 4*t^7.286 + 3*t^7.714 + 2*t^8.571 - t^4.286/y + (2*t^8.143)/y + (4*t^8.571)/y - t^4.286*y + 2*t^8.143*y + 4*t^8.571*y |
Deformation
Here is the data for the deformed fixed points from the chosen fixed point.
# | Superpotential | Central Charge $a$ | Central Charge $c$ | Ratio $a/c$ | $R$-charges | Superconformal Index | More Info. | Rational |
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Equivalent Fixed Points from Other Seed Theories
Here is a list of equivalent fixed points from other gauge theories.
# | Theory | Superpotential | Central Charge $a$ | Central Charge $c$ | Ratio $a/c$ | $R$-charges | Superconformal Index | More Info. | Rational |
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Equivalent Fixed Points from the Same Seed Theory
Below is a list of equivalent fixed points from the same seed theories.
id | Theory | Superpotential | Central Charge $a$ | Central Charge $c$ | Ratio $a/c$ | $R$-charges | More Info. | Rational |
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Previous Theory
The previous fixed point before deforming to get the chosen fixed point.
# | Theory | Superpotential | Central Charge $a$ | Central Charge $c$ | Ratio $a/c$ | $R$-charges | Superconformal Index | More Info. | Rational |
---|---|---|---|---|---|---|---|---|---|
47191 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}q_{1}\tilde{q}_{1}$ + ${ }M_{3}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{3}M_{4}$ + ${ }\phi_{1}^{2}q_{2}\tilde{q}_{1}$ + ${ }M_{5}\phi_{1}^{2}$ + ${ }\phi_{1}q_{1}\tilde{q}_{1}$ + ${ }M_{2}X_{1}$ | 0.6022 | 0.7272 | 0.8281 | [X:[1.6128], M:[0.7104, 0.3872, 0.8384, 1.1616, 1.2256], q:[0.8384, 0.4512], qb:[0.7744, 0.3872], phi:[0.3872]] | t^2.131 + t^2.515 + 2*t^3.485 + 4*t^3.677 + t^3.869 + t^4.263 + t^4.646 + t^4.838 + t^5.03 + 2*t^5.616 + 2*t^5.808 - 2*t^6. - t^4.162/y - t^4.162*y | detail |