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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4654 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{3}q_{1}\tilde{q}_{1}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{5}q_{2}\tilde{q}_{1}$ + ${ }M_{4}M_{5}$ + ${ }M_{1}\phi_{1}^{2}$ + ${ }M_{6}q_{1}\tilde{q}_{2}$ + ${ }M_{7}\phi_{1}q_{2}^{2}$ + ${ }M_{1}M_{8}$ + ${ }M_{7}^{2}$ + ${ }M_{2}X_{1}$ | 0.6522 | 0.8218 | 0.7936 | [X:[1.4286], M:[1.1429, 0.5714, 0.7143, 1.0, 1.0, 0.7143, 1.0, 0.8571], q:[0.5714, 0.2857], qb:[0.7143, 0.7143], phi:[0.4286]] | [X:[[0]], M:[[0], [0], [1], [-1], [1], [-1], [0], [0]], q:[[0], [0]], qb:[[-1], [1]], phi:[[0]]] | 1 | {a: 3579/5488, c: 2255/2744, X1: 10/7, M1: 8/7, M2: 4/7, M3: 5/7, M4: 1, M5: 1, M6: 5/7, M7: 1, M8: 6/7, q1: 4/7, q2: 2/7, qb1: 5/7, qb2: 5/7, phi1: 3/7} |
Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
---|---|---|---|---|
${}M_{6}$, ${ }M_{3}$, ${ }M_{8}$, ${ }\phi_{1}^{2}$, ${ }M_{4}$, ${ }M_{5}$, ${ }M_{7}$, ${ }M_{4}$, ${ }M_{5}$, ${ }\phi_{1}q_{1}q_{2}$, ${ }M_{3}^{2}$, ${ }M_{3}M_{6}$, ${ }M_{6}^{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }X_{1}$, ${ }M_{6}^{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }M_{3}^{2}$, ${ }M_{3}M_{8}$, ${ }M_{6}M_{8}$, ${ }M_{3}\phi_{1}^{2}$, ${ }M_{6}\phi_{1}^{2}$, ${ }\phi_{1}q_{1}^{2}$, ${ }M_{6}M_{8}$, ${ }M_{6}\phi_{1}^{2}$, ${ }M_{3}M_{8}$, ${ }M_{3}\phi_{1}^{2}$, ${ }M_{3}M_{4}$, ${ }M_{3}M_{5}$, ${ }M_{4}M_{6}$, ${ }M_{5}M_{6}$, ${ }M_{3}M_{7}$, ${ }M_{6}M_{7}$, ${ }M_{8}^{2}$, ${ }M_{8}\phi_{1}^{2}$, ${ }\phi_{1}^{4}$, ${ }\phi_{1}q_{1}\tilde{q}_{1}$, ${ }\phi_{1}q_{1}\tilde{q}_{2}$, ${ }M_{4}M_{6}$, ${ }M_{6}M_{7}$, ${ }\phi_{1}q_{1}\tilde{q}_{1}$, ${ }M_{3}M_{7}$, ${ }\phi_{1}q_{1}\tilde{q}_{2}$, ${ }M_{3}M_{5}$, ${ }M_{4}M_{8}$, ${ }M_{5}M_{8}$, ${ }M_{7}M_{8}$, ${ }M_{4}\phi_{1}^{2}$, ${ }M_{5}\phi_{1}^{2}$, ${ }M_{7}\phi_{1}^{2}$, ${ }\phi_{1}\tilde{q}_{1}^{2}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$, ${ }\phi_{1}\tilde{q}_{2}^{2}$, ${ }\phi_{1}\tilde{q}_{1}^{2}$, ${ }M_{4}M_{8}$, ${ }M_{4}\phi_{1}^{2}$, ${ }M_{5}M_{8}$, ${ }M_{5}\phi_{1}^{2}$, ${ }\phi_{1}\tilde{q}_{2}^{2}$ | ${}M_{4}^{2}$, ${ }M_{5}^{2}$, ${ }M_{4}M_{7}$, ${ }M_{5}M_{7}$, ${ }M_{3}\phi_{1}q_{1}q_{2}$, ${ }M_{6}\phi_{1}q_{1}q_{2}$ | 0 | 2*t^2.143 + 2*t^2.571 + 3*t^3. + t^3.857 + 6*t^4.286 + 3*t^4.714 + 10*t^5.143 + 7*t^5.571 + 8*t^6.429 + 7*t^6.857 + 15*t^7.286 + 14*t^7.714 + 9*t^8.143 + 11*t^8.571 - t^4.286/y - (2*t^6.429)/y - t^6.857/y + t^7.286/y + (5*t^7.714)/y + (9*t^8.143)/y + (3*t^8.571)/y - t^4.286*y - 2*t^6.429*y - t^6.857*y + t^7.286*y + 5*t^7.714*y + 9*t^8.143*y + 3*t^8.571*y | t^2.143/g1 + g1*t^2.143 + 2*t^2.571 + t^3. + t^3./g1 + g1*t^3. + t^3.857 + 2*t^4.286 + t^4.286/g1^2 + t^4.286/g1 + g1*t^4.286 + g1^2*t^4.286 + t^4.714 + t^4.714/g1 + g1*t^4.714 + 4*t^5.143 + t^5.143/g1^2 + (2*t^5.143)/g1 + 2*g1*t^5.143 + g1^2*t^5.143 + 3*t^5.571 + t^5.571/g1^2 + t^5.571/g1 + g1*t^5.571 + g1^2*t^5.571 - 2*t^6. + t^6./g1 + g1*t^6. + 2*t^6.429 + t^6.429/g1^3 + t^6.429/g1^2 + t^6.429/g1 + g1*t^6.429 + g1^2*t^6.429 + g1^3*t^6.429 + t^6.857 + t^6.857/g1^2 + (2*t^6.857)/g1 + 2*g1*t^6.857 + g1^2*t^6.857 + 3*t^7.286 + t^7.286/g1^3 + (2*t^7.286)/g1^2 + (3*t^7.286)/g1 + 3*g1*t^7.286 + 2*g1^2*t^7.286 + g1^3*t^7.286 + 4*t^7.714 + t^7.714/g1^3 + t^7.714/g1^2 + (3*t^7.714)/g1 + 3*g1*t^7.714 + g1^2*t^7.714 + g1^3*t^7.714 + 3*t^8.143 + (3*t^8.143)/g1^2 + 3*g1^2*t^8.143 - t^8.571 + t^8.571/g1^4 + (2*t^8.571)/g1^3 + (2*t^8.571)/g1^2 + t^8.571/g1 + g1*t^8.571 + 2*g1^2*t^8.571 + 2*g1^3*t^8.571 + g1^4*t^8.571 - t^4.286/y - t^6.429/(g1*y) - (g1*t^6.429)/y - t^6.857/y + t^7.286/y + t^7.714/y + (2*t^7.714)/(g1*y) + (2*g1*t^7.714)/y + (3*t^8.143)/y + t^8.143/(g1^2*y) + (2*t^8.143)/(g1*y) + (2*g1*t^8.143)/y + (g1^2*t^8.143)/y + t^8.571/y - t^8.571/(g1^2*y) + (2*t^8.571)/(g1*y) + (2*g1*t^8.571)/y - (g1^2*t^8.571)/y - t^4.286*y - (t^6.429*y)/g1 - g1*t^6.429*y - t^6.857*y + t^7.286*y + t^7.714*y + (2*t^7.714*y)/g1 + 2*g1*t^7.714*y + 3*t^8.143*y + (t^8.143*y)/g1^2 + (2*t^8.143*y)/g1 + 2*g1*t^8.143*y + g1^2*t^8.143*y + t^8.571*y - (t^8.571*y)/g1^2 + (2*t^8.571*y)/g1 + 2*g1*t^8.571*y - g1^2*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 |
---|---|---|---|---|---|---|---|---|
6194 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{3}q_{1}\tilde{q}_{1}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{5}q_{2}\tilde{q}_{1}$ + ${ }M_{4}M_{5}$ + ${ }M_{1}\phi_{1}^{2}$ + ${ }M_{6}q_{1}\tilde{q}_{2}$ + ${ }M_{7}\phi_{1}q_{2}^{2}$ + ${ }M_{1}M_{8}$ + ${ }M_{7}^{2}$ + ${ }M_{2}X_{1}$ + ${ }M_{8}M_{9}$ | 0.6396 | 0.8003 | 0.7992 | [X:[1.4286], M:[1.1429, 0.5714, 0.7143, 1.0, 1.0, 0.7143, 1.0, 0.8571, 1.1429], q:[0.5714, 0.2857], qb:[0.7143, 0.7143], phi:[0.4286]] | 2*t^2.143 + t^2.571 + 3*t^3. + t^3.429 + t^3.857 + 6*t^4.286 + t^4.714 + 8*t^5.143 + 6*t^5.571 + t^6. - t^4.286/y - t^4.286*y | detail | {a: 1755/2744, c: 549/686, X1: 10/7, M1: 8/7, M2: 4/7, M3: 5/7, M4: 1, M5: 1, M6: 5/7, M7: 1, M8: 6/7, M9: 8/7, q1: 4/7, q2: 2/7, qb1: 5/7, qb2: 5/7, phi1: 3/7} |
6198 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{3}q_{1}\tilde{q}_{1}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{5}q_{2}\tilde{q}_{1}$ + ${ }M_{4}M_{5}$ + ${ }M_{1}\phi_{1}^{2}$ + ${ }M_{6}q_{1}\tilde{q}_{2}$ + ${ }M_{7}\phi_{1}q_{2}^{2}$ + ${ }M_{1}M_{8}$ + ${ }M_{7}^{2}$ + ${ }M_{2}X_{1}$ + ${ }M_{9}\phi_{1}q_{1}q_{2}$ | 0.6724 | 0.8599 | 0.7819 | [X:[1.4286], M:[1.1429, 0.5714, 0.7143, 1.0, 1.0, 0.7143, 1.0, 0.8571, 0.7143], q:[0.5714, 0.2857], qb:[0.7143, 0.7143], phi:[0.4286]] | 3*t^2.143 + 2*t^2.571 + 3*t^3. + 9*t^4.286 + 5*t^4.714 + 13*t^5.143 + 7*t^5.571 - 2*t^6. - t^4.286/y - t^4.286*y | detail | {a: 1845/2744, c: 4719/5488, X1: 10/7, M1: 8/7, M2: 4/7, M3: 5/7, M4: 1, M5: 1, M6: 5/7, M7: 1, M8: 6/7, M9: 5/7, q1: 4/7, q2: 2/7, qb1: 5/7, qb2: 5/7, phi1: 3/7} |
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 |
---|---|---|---|---|---|---|---|---|---|
2568 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{3}q_{1}\tilde{q}_{1}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{5}q_{2}\tilde{q}_{1}$ + ${ }M_{4}M_{5}$ + ${ }M_{1}\phi_{1}^{2}$ + ${ }M_{6}q_{1}\tilde{q}_{2}$ + ${ }M_{7}\phi_{1}q_{2}^{2}$ + ${ }M_{1}M_{8}$ | 0.7441 | 0.9354 | 0.7955 | [M:[1.0606, 0.8183, 0.8789, 1.0, 1.0, 0.8789, 0.7119, 0.9394], q:[0.5303, 0.4092], qb:[0.5908, 0.5908], phi:[0.4697]] | t^2.136 + t^2.455 + 2*t^2.637 + 2*t^2.818 + 2*t^3. + t^4.228 + t^4.272 + 2*t^4.409 + 2*t^4.591 + 4*t^4.772 + t^4.91 + 5*t^4.954 + 2*t^5.092 + 2*t^5.136 + 5*t^5.273 + 4*t^5.455 + 6*t^5.637 + 2*t^5.818 - 3*t^6. - t^4.409/y - t^4.409*y | detail |