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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58153 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}q_{1}\tilde{q}_{1}$ + ${ }M_{3}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{5}q_{1}\tilde{q}_{2}$ + ${ }M_{6}q_{2}\tilde{q}_{1}$ + ${ }M_{3}^{2}$ + ${ }M_{1}M_{2}$ + ${ }M_{4}M_{5}$ + ${ }M_{7}\phi_{1}^{2}$ + ${ }M_{5}M_{8}$ | 0.7018 | 0.8654 | 0.8109 | [M:[0.9637, 1.0363, 1.0, 0.9274, 1.0726, 0.8912, 1.0181, 0.9274], q:[0.4456, 0.5907], qb:[0.5181, 0.4819], phi:[0.4909]] | [M:[[4], [-4], [0], [8], [-8], [12], [-2], [8]], q:[[6], [-10]], qb:[[-2], [2]], phi:[[1]]] | 1 |
Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
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${}M_{6}$, ${ }M_{4}$, ${ }M_{8}$, ${ }M_{1}$, ${ }M_{3}$, ${ }M_{7}$, ${ }M_{2}$, ${ }\phi_{1}q_{1}^{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{1}$, ${ }\phi_{1}\tilde{q}_{2}^{2}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$, ${ }\phi_{1}q_{1}q_{2}$, ${ }\phi_{1}\tilde{q}_{1}^{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}q_{2}^{2}$, ${ }M_{6}^{2}$, ${ }M_{4}M_{6}$, ${ }M_{6}M_{8}$, ${ }M_{4}^{2}$, ${ }M_{1}M_{6}$, ${ }M_{4}M_{8}$, ${ }M_{8}^{2}$, ${ }M_{1}M_{4}$, ${ }M_{3}M_{6}$, ${ }M_{1}M_{8}$, ${ }M_{6}M_{7}$, ${ }M_{1}^{2}$, ${ }M_{3}M_{4}$, ${ }M_{2}M_{6}$, ${ }M_{3}M_{8}$, ${ }M_{4}M_{7}$, ${ }M_{7}M_{8}$, ${ }M_{1}M_{3}$, ${ }M_{2}M_{4}$, ${ }M_{2}M_{8}$, ${ }M_{1}M_{7}$ | ${}$ | -2 | t^2.673 + 2*t^2.782 + t^2.891 + t^3. + t^3.054 + t^3.109 + t^4.146 + t^4.255 + 2*t^4.364 + t^4.473 + 2*t^4.582 + t^4.69 + t^4.799 + t^5.017 + t^5.347 + 2*t^5.456 + 3*t^5.565 + 2*t^5.673 + t^5.728 + 2*t^5.782 + 2*t^5.837 + t^5.891 + t^5.946 - 2*t^6. + t^6.054 - t^6.109 + t^6.163 - t^6.218 - t^6.327 - t^6.435 + t^6.82 + 3*t^6.929 + 4*t^7.037 + 5*t^7.146 + 5*t^7.255 + 5*t^7.364 + 3*t^7.473 + t^7.582 + t^7.69 + t^7.799 + t^8.02 + t^8.126 + 2*t^8.129 + 3*t^8.238 + t^8.292 + 4*t^8.347 + 2*t^8.401 + 3*t^8.456 + 4*t^8.51 + t^8.565 + 5*t^8.619 - 3*t^8.673 + 6*t^8.728 - 7*t^8.782 + 5*t^8.837 - 6*t^8.891 + 5*t^8.946 - t^4.473/y - t^7.146/y - t^7.255/y + t^7.69/y + t^7.799/y + (2*t^8.456)/y + (2*t^8.565)/y + (3*t^8.673)/y + t^8.728/y + (3*t^8.782)/y + (2*t^8.837)/y + (3*t^8.891)/y + t^8.946/y - t^4.473*y - t^7.146*y - t^7.255*y + t^7.69*y + t^7.799*y + 2*t^8.456*y + 2*t^8.565*y + 3*t^8.673*y + t^8.728*y + 3*t^8.782*y + 2*t^8.837*y + 3*t^8.891*y + t^8.946*y | g1^12*t^2.673 + 2*g1^8*t^2.782 + g1^4*t^2.891 + t^3. + t^3.054/g1^2 + t^3.109/g1^4 + g1^13*t^4.146 + g1^9*t^4.255 + 2*g1^5*t^4.364 + g1*t^4.473 + (2*t^4.582)/g1^3 + t^4.69/g1^7 + t^4.799/g1^11 + t^5.017/g1^19 + g1^24*t^5.347 + 2*g1^20*t^5.456 + 3*g1^16*t^5.565 + 2*g1^12*t^5.673 + g1^10*t^5.728 + 2*g1^8*t^5.782 + 2*g1^6*t^5.837 + g1^4*t^5.891 + g1^2*t^5.946 - 2*t^6. + t^6.054/g1^2 - t^6.109/g1^4 + t^6.163/g1^6 - t^6.218/g1^8 - t^6.327/g1^12 - t^6.435/g1^16 + g1^25*t^6.82 + 3*g1^21*t^6.929 + 4*g1^17*t^7.037 + 5*g1^13*t^7.146 + 5*g1^9*t^7.255 + 5*g1^5*t^7.364 + 3*g1*t^7.473 + t^7.582/g1^3 + t^7.69/g1^7 + t^7.799/g1^11 + g1^36*t^8.02 + t^8.126/g1^23 + 2*g1^32*t^8.129 + 3*g1^28*t^8.238 + g1^26*t^8.292 + 4*g1^24*t^8.347 + 2*g1^22*t^8.401 + 3*g1^20*t^8.456 + 4*g1^18*t^8.51 + g1^16*t^8.565 + 5*g1^14*t^8.619 - 3*g1^12*t^8.673 + 6*g1^10*t^8.728 - 7*g1^8*t^8.782 + 5*g1^6*t^8.837 - 6*g1^4*t^8.891 + 5*g1^2*t^8.946 - (g1*t^4.473)/y - (g1^13*t^7.146)/y - (g1^9*t^7.255)/y + t^7.69/(g1^7*y) + t^7.799/(g1^11*y) + (2*g1^20*t^8.456)/y + (2*g1^16*t^8.565)/y + (3*g1^12*t^8.673)/y + (g1^10*t^8.728)/y + (3*g1^8*t^8.782)/y + (2*g1^6*t^8.837)/y + (3*g1^4*t^8.891)/y + (g1^2*t^8.946)/y - g1*t^4.473*y - g1^13*t^7.146*y - g1^9*t^7.255*y + (t^7.69*y)/g1^7 + (t^7.799*y)/g1^11 + 2*g1^20*t^8.456*y + 2*g1^16*t^8.565*y + 3*g1^12*t^8.673*y + g1^10*t^8.728*y + 3*g1^8*t^8.782*y + 2*g1^6*t^8.837*y + 3*g1^4*t^8.891*y + g1^2*t^8.946*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 |
---|---|---|---|---|---|---|---|---|---|
56015 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}q_{1}\tilde{q}_{1}$ + ${ }M_{3}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{5}q_{1}\tilde{q}_{2}$ + ${ }M_{6}q_{2}\tilde{q}_{1}$ + ${ }M_{3}^{2}$ + ${ }M_{1}M_{2}$ + ${ }M_{4}M_{5}$ + ${ }M_{7}\phi_{1}^{2}$ | 0.6961 | 0.8543 | 0.8148 | [M:[0.9753, 1.0247, 1.0, 0.9505, 1.0495, 0.9258, 1.0124], q:[0.4629, 0.5618], qb:[0.5124, 0.4876], phi:[0.4938]] | t^2.777 + t^2.852 + t^2.926 + t^3. + t^3.037 + t^3.074 + t^3.148 + t^4.259 + t^4.333 + 2*t^4.407 + t^4.481 + 2*t^4.556 + t^4.63 + t^4.704 + t^4.853 + t^5.555 + t^5.629 + t^5.703 + t^5.777 + t^5.814 + t^5.852 + t^5.889 + t^5.926 + t^5.963 - t^6. - t^4.481/y - t^4.481*y | detail |