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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55709 | SU2adj1nf3 | ${}\phi_{1}q_{1}q_{2}$ + ${ }M_{1}q_{2}q_{3}$ + ${ }M_{1}q_{1}\tilde{q}_{1}$ + ${ }\phi_{1}\tilde{q}_{2}\tilde{q}_{3}$ | 0.8159 | 0.9874 | 0.8264 | [M:[0.7471], q:[0.751, 0.751, 0.5019], qb:[0.5019, 0.751, 0.751], phi:[0.4981]] | [M:[[0, -3, -3]], q:[[-1, 3, 3], [1, -1, -1], [-1, 4, 4]], qb:[[1, 0, 0], [0, 2, 0], [0, 0, 2]], phi:[[0, -2, -2]]] | 3 |
Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
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${}M_{1}$, ${ }\phi_{1}^{2}$, ${ }q_{3}\tilde{q}_{1}$, ${ }\tilde{q}_{1}\tilde{q}_{2}$, ${ }q_{2}\tilde{q}_{1}$, ${ }\tilde{q}_{1}\tilde{q}_{3}$, ${ }q_{1}\tilde{q}_{1}$, ${ }q_{3}\tilde{q}_{2}$, ${ }q_{3}\tilde{q}_{3}$, ${ }q_{1}q_{3}$, ${ }M_{1}^{2}$, ${ }\phi_{1}\tilde{q}_{1}^{2}$, ${ }q_{2}\tilde{q}_{2}$, ${ }q_{2}\tilde{q}_{3}$, ${ }q_{1}q_{2}$, ${ }\phi_{1}q_{3}\tilde{q}_{1}$, ${ }\tilde{q}_{2}\tilde{q}_{3}$, ${ }q_{1}\tilde{q}_{2}$, ${ }q_{1}\tilde{q}_{3}$, ${ }\phi_{1}q_{3}^{2}$, ${ }M_{1}\phi_{1}^{2}$, ${ }M_{1}q_{3}\tilde{q}_{1}$, ${ }\phi_{1}^{4}$ | ${}\phi_{1}^{2}q_{3}\tilde{q}_{1}$, ${ }M_{1}q_{3}\tilde{q}_{2}$, ${ }M_{1}\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{1}q_{3}\tilde{q}_{3}$, ${ }M_{1}\tilde{q}_{1}\tilde{q}_{3}$ | -2 | t^2.241 + t^2.989 + t^3.011 + 7*t^3.759 + t^4.483 + 9*t^4.506 + t^5.23 + t^5.253 + t^5.977 - 2*t^6. + t^6.023 + t^6.724 + 7*t^6.77 + t^7.471 + t^7.494 + 28*t^7.517 + t^8.219 - 2*t^8.241 + 40*t^8.264 + 2*t^8.966 - t^4.494/y - t^6.736/y - t^7.483/y + t^7.506/y + t^8.23/y + (2*t^8.253)/y - t^8.977/y - t^4.494*y - t^6.736*y - t^7.483*y + t^7.506*y + t^8.23*y + 2*t^8.253*y - t^8.977*y | t^2.241/(g2^3*g3^3) + t^2.989/(g2^4*g3^4) + g2^4*g3^4*t^3.011 + g1*g2^2*t^3.759 + (g1^2*t^3.759)/(g2*g3) + g1*g3^2*t^3.759 + g2^3*g3^3*t^3.759 + (g2^6*g3^4*t^3.759)/g1 + (g2^4*g3^6*t^3.759)/g1 + (g2^7*g3^7*t^3.759)/g1^2 + t^4.483/(g2^6*g3^6) + (g1^2*t^4.506)/(g2^2*g3^2) + (g1*g2*t^4.506)/g3 + (g1*g3*t^4.506)/g2 + 3*g2^2*g3^2*t^4.506 + (g2^5*g3^3*t^4.506)/g1 + (g2^3*g3^5*t^4.506)/g1 + (g2^6*g3^6*t^4.506)/g1^2 + t^5.23/(g2^7*g3^7) + g2*g3*t^5.253 + t^5.977/(g2^8*g3^8) - 2*t^6. + g2^8*g3^8*t^6.023 + t^6.724/(g2^9*g3^9) + g1^2*g2^3*g3^3*t^6.77 + g1*g2^6*g3^4*t^6.77 + g1*g2^4*g3^6*t^6.77 + g2^7*g3^7*t^6.77 + (g2^10*g3^8*t^6.77)/g1 + (g2^8*g3^10*t^6.77)/g1 + (g2^11*g3^11*t^6.77)/g1^2 + t^7.471/(g2^10*g3^10) + t^7.494/(g2^2*g3^2) + g1^2*g2^4*t^7.517 + (g1^4*t^7.517)/(g2^2*g3^2) + (g1^3*g2*t^7.517)/g3 + (g1^3*g3*t^7.517)/g2 + 2*g1^2*g2^2*g3^2*t^7.517 + 2*g1*g2^5*g3^3*t^7.517 + g1^2*g3^4*t^7.517 + g2^8*g3^4*t^7.517 + 2*g1*g2^3*g3^5*t^7.517 + 4*g2^6*g3^6*t^7.517 + (2*g2^9*g3^7*t^7.517)/g1 + g2^4*g3^8*t^7.517 + (g2^12*g3^8*t^7.517)/g1^2 + (2*g2^7*g3^9*t^7.517)/g1 + (2*g2^10*g3^10*t^7.517)/g1^2 + (g2^13*g3^11*t^7.517)/g1^3 + (g2^8*g3^12*t^7.517)/g1^2 + (g2^11*g3^13*t^7.517)/g1^3 + (g2^14*g3^14*t^7.517)/g1^4 + t^8.219/(g2^11*g3^11) - (2*t^8.241)/(g2^3*g3^3) + (2*g1^3*t^8.264)/g2^2 + (g1^4*t^8.264)/(g2^3*g3^3) + (2*g1^3*t^8.264)/g3^2 + (g1^2*g2^3*t^8.264)/g3 + 3*g1^2*g2*g3*t^8.264 + 3*g1*g2^4*g3^2*t^8.264 + (g1^2*g3^3*t^8.264)/g2 + 2*g2^7*g3^3*t^8.264 + 3*g1*g2^2*g3^4*t^8.264 + 4*g2^5*g3^5*t^8.264 + (3*g2^8*g3^6*t^8.264)/g1 + 2*g2^3*g3^7*t^8.264 + (g2^11*g3^7*t^8.264)/g1^2 + (3*g2^6*g3^8*t^8.264)/g1 + (3*g2^9*g3^9*t^8.264)/g1^2 + (2*g2^12*g3^10*t^8.264)/g1^3 + (g2^7*g3^11*t^8.264)/g1^2 + (2*g2^10*g3^12*t^8.264)/g1^3 + (g2^13*g3^13*t^8.264)/g1^4 + (2*t^8.966)/(g2^12*g3^12) - t^4.494/(g2^2*g3^2*y) - t^6.736/(g2^5*g3^5*y) - t^7.483/(g2^6*g3^6*y) + (g2^2*g3^2*t^7.506)/y + t^8.23/(g2^7*g3^7*y) + (2*g2*g3*t^8.253)/y - t^8.977/(g2^8*g3^8*y) - (t^4.494*y)/(g2^2*g3^2) - (t^6.736*y)/(g2^5*g3^5) - (t^7.483*y)/(g2^6*g3^6) + g2^2*g3^2*t^7.506*y + (t^8.23*y)/(g2^7*g3^7) + 2*g2*g3*t^8.253*y - (t^8.977*y)/(g2^8*g3^8) |
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 |
---|---|---|---|---|---|---|---|---|---|
55600 | SU2adj1nf3 | ${}\phi_{1}q_{1}q_{2}$ + ${ }M_{1}q_{2}q_{3}$ + ${ }M_{1}q_{1}\tilde{q}_{1}$ | 0.8641 | 1.0549 | 0.8192 | [M:[0.6821], q:[0.7266, 0.7266, 0.5914], qb:[0.5914, 0.5883, 0.5883], phi:[0.5469]] | t^2.046 + t^3.281 + t^3.53 + 4*t^3.539 + t^3.548 + 4*t^3.945 + 3*t^3.954 + t^4.092 + t^4.359 + 3*t^5.17 + 4*t^5.18 + 3*t^5.189 + t^5.328 + t^5.576 + 4*t^5.585 + t^5.594 - 6*t^6. - t^4.641/y - t^4.641*y | detail |