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 |
---|---|---|---|---|---|---|---|---|---|
55539 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}q_{1}\tilde{q}_{1}$ + ${ }\phi_{1}q_{1}\tilde{q}_{2}$ + ${ }M_{1}M_{2}$ + ${ }M_{3}\phi_{1}\tilde{q}_{1}^{2}$ + ${ }M_{3}^{2}$ + ${ }q_{2}\tilde{q}_{1}^{2}\tilde{q}_{2}$ + ${ }M_{1}M_{4}$ + ${ }M_{5}\phi_{1}^{2}$ | 0.5306 | 0.6452 | 0.8224 | [M:[0.9167, 1.0833, 1.0, 1.0833, 1.1667], q:[0.625, 0.4583], qb:[0.2917, 0.9583], phi:[0.4167]] | [M:[[0], [0], [0], [0], [0]], q:[[0], [0]], qb:[[0], [0]], phi:[[0]]] | 0 | {a: 815/1536, c: 991/1536, M1: 11/12, M2: 13/12, M3: 1, M4: 13/12, M5: 7/6, q1: 5/8, q2: 11/24, qb1: 7/24, qb2: 23/24, phi1: 5/12} |
Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
---|---|---|---|---|
${}q_{2}\tilde{q}_{1}$, ${ }M_{3}$, ${ }M_{2}$, ${ }M_{4}$, ${ }M_{5}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }\tilde{q}_{1}\tilde{q}_{2}$, ${ }\phi_{1}q_{2}^{2}$, ${ }q_{2}\tilde{q}_{2}$, ${ }q_{2}^{2}\tilde{q}_{1}^{2}$, ${ }q_{1}\tilde{q}_{2}$, ${ }M_{2}q_{2}\tilde{q}_{1}$, ${ }M_{4}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }M_{5}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}q_{2}^{2}\tilde{q}_{1}^{2}$ | ${}$ | -1 | t^2.25 + t^3. + 2*t^3.25 + 2*t^3.5 + t^3.75 + t^4. + t^4.25 + t^4.5 + t^4.75 + t^5.5 + t^5.75 - t^6. + t^6.25 + 3*t^6.5 + 3*t^6.75 + 3*t^7. + 2*t^7.25 + 2*t^7.5 + 2*t^7.75 + 3*t^8. - t^8.25 - t^4.25/y + t^7./y - t^7.5/y + t^8.25/y + (2*t^8.5)/y + (2*t^8.75)/y - t^4.25*y + t^7.*y - t^7.5*y + t^8.25*y + 2*t^8.5*y + 2*t^8.75*y | t^2.25 + t^3. + 2*t^3.25 + 2*t^3.5 + t^3.75 + t^4. + t^4.25 + t^4.5 + t^4.75 + t^5.5 + t^5.75 - t^6. + t^6.25 + 3*t^6.5 + 3*t^6.75 + 3*t^7. + 2*t^7.25 + 2*t^7.5 + 2*t^7.75 + 3*t^8. - t^8.25 - t^4.25/y + t^7./y - t^7.5/y + t^8.25/y + (2*t^8.5)/y + (2*t^8.75)/y - t^4.25*y + t^7.*y - t^7.5*y + t^8.25*y + 2*t^8.5*y + 2*t^8.75*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 |
---|---|---|---|---|---|---|---|---|---|
47254 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}q_{1}\tilde{q}_{1}$ + ${ }\phi_{1}q_{1}\tilde{q}_{2}$ + ${ }M_{1}M_{2}$ + ${ }M_{3}\phi_{1}\tilde{q}_{1}^{2}$ + ${ }M_{3}^{2}$ + ${ }q_{2}\tilde{q}_{1}^{2}\tilde{q}_{2}$ + ${ }M_{1}M_{4}$ | 0.5449 | 0.6699 | 0.8134 | [M:[0.9167, 1.0833, 1.0, 1.0833], q:[0.625, 0.4583], qb:[0.2917, 0.9583], phi:[0.4167]] | t^2.25 + t^2.5 + t^3. + 2*t^3.25 + t^3.5 + t^3.75 + t^4. + t^4.25 + t^4.5 + 2*t^4.75 + t^5. + 2*t^5.5 + 2*t^5.75 - t^4.25/y - t^4.25*y | detail | {a: 279/512, c: 343/512, M1: 11/12, M2: 13/12, M3: 1, M4: 13/12, q1: 5/8, q2: 11/24, qb1: 7/24, qb2: 23/24, phi1: 5/12} |