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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58089 | SU3adj1nf2 | ${}q_{1}^{2}\tilde{q}_{1}^{2}$ + ${ }q_{2}^{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }\phi_{1}^{2}X_{1}$ + ${ }M_{1}q_{1}\tilde{q}_{2}$ + ${ }M_{2}\phi_{1}q_{1}\tilde{q}_{1}$ | 1.4758 | 1.6839 | 0.8764 | [X:[1.3409], M:[0.9545, 0.6705], q:[0.5169, 0.4941], qb:[0.4831, 0.5287], phi:[0.3295]] | [X:[[0, 2]], M:[[0, -12], [0, 1]], q:[[-1, 12], [-1, 6]], qb:[[1, -12], [1, 0]], phi:[[0, -1]]] | 2 |
Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
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${}M_{2}$, ${ }M_{1}$, ${ }q_{2}\tilde{q}_{1}$, ${ }\phi_{1}^{3}$, ${ }q_{1}\tilde{q}_{1}$, ${ }q_{2}\tilde{q}_{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }M_{2}^{2}$, ${ }X_{1}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{2}$, ${ }M_{1}M_{2}$, ${ }\phi_{1}^{2}q_{2}\tilde{q}_{1}$, ${ }M_{2}q_{2}\tilde{q}_{1}$, ${ }M_{2}\phi_{1}^{3}$, ${ }\phi_{1}^{2}q_{1}\tilde{q}_{1}$, ${ }M_{2}q_{1}\tilde{q}_{1}$, ${ }\phi_{1}^{2}q_{2}\tilde{q}_{2}$, ${ }M_{2}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}^{2}q_{1}\tilde{q}_{2}$, ${ }\phi_{1}\tilde{q}_{1}^{2}\tilde{q}_{2}$, ${ }\phi_{1}q_{1}q_{2}^{2}$, ${ }\phi_{1}q_{1}^{2}q_{2}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}^{2}$, ${ }M_{1}^{2}$, ${ }M_{1}q_{2}\tilde{q}_{1}$, ${ }M_{1}\phi_{1}^{3}$, ${ }M_{1}q_{1}\tilde{q}_{1}$, ${ }\phi_{1}^{3}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}^{6}$, ${ }M_{2}\phi_{1}q_{2}\tilde{q}_{1}$, ${ }M_{1}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}^{3}q_{1}\tilde{q}_{1}$ | ${}$ | -2 | t^2.01 + t^2.86 + t^2.93 + t^2.97 + t^3. + t^3.07 + t^3.92 + 2*t^4.02 + t^4.06 + t^4.13 + t^4.87 + t^4.91 + t^4.94 + 2*t^4.98 + t^5.01 + t^5.05 + t^5.08 + t^5.11 + t^5.47 + t^5.5 + t^5.57 + t^5.61 + t^5.73 + t^5.8 + t^5.83 + t^5.86 + t^5.9 + 3*t^5.93 + t^5.97 - 2*t^6. + 3*t^6.03 + t^6.07 + t^6.14 + t^6.46 + t^6.49 + t^6.56 + t^6.6 + t^6.78 + 3*t^6.89 + 2*t^6.92 + 2*t^6.95 + 3*t^6.99 + 3*t^7.02 + 2*t^7.06 + 3*t^7.09 + 2*t^7.13 + t^7.19 + t^7.31 + t^7.41 + t^7.48 + t^7.52 + t^7.59 + 2*t^7.62 + t^7.72 + t^7.74 + t^7.77 + t^7.81 + 3*t^7.84 + 2*t^7.87 + 3*t^7.91 + 4*t^7.94 + 4*t^7.98 - 2*t^8.01 + 6*t^8.05 + 2*t^8.08 + 2*t^8.11 + t^8.15 + 2*t^8.18 + t^8.25 + t^8.44 + 2*t^8.47 + t^8.5 + t^8.54 + t^8.57 + t^8.58 + t^8.59 + t^8.61 + t^8.66 + t^8.69 + t^8.73 + t^8.76 + 3*t^8.8 + 2*t^8.83 - t^8.86 + 6*t^8.9 + 3*t^8.97 + t^8.97/y^2 - t^3.99/y - t^4.98/y - t^6./y - t^6.85/y - t^6.92/y - t^6.95/y - (2*t^6.99)/y - t^7.06/y - t^7.84/y + t^7.87/y - t^7.91/y + t^7.98/y - t^8.05/y + t^8.08/y + t^8.8/y + t^8.83/y + (2*t^8.93)/y - t^3.99*y - t^4.98*y - t^6.*y - t^6.85*y - t^6.92*y - t^6.95*y - 2*t^6.99*y - t^7.06*y - t^7.84*y + t^7.87*y - t^7.91*y + t^7.98*y - t^8.05*y + t^8.08*y + t^8.8*y + t^8.83*y + 2*t^8.93*y + t^8.97*y^2 | g2*t^2.01 + t^2.86/g2^12 + t^2.93/g2^6 + t^2.97/g2^3 + t^3. + g2^6*t^3.07 + t^3.92/g2^7 + 2*g2^2*t^4.02 + g2^5*t^4.06 + g2^11*t^4.13 + t^4.87/g2^11 + t^4.91/g2^8 + t^4.94/g2^5 + (2*t^4.98)/g2^2 + g2*t^5.01 + g2^4*t^5.05 + g2^7*t^5.08 + g2^10*t^5.11 + (g1^3*t^5.47)/g2^25 + (g2^23*t^5.5)/g1^3 + (g2^29*t^5.57)/g1^3 + (g1^3*t^5.61)/g2^13 + t^5.73/g2^24 + t^5.8/g2^18 + t^5.83/g2^15 + t^5.86/g2^12 + t^5.9/g2^9 + (3*t^5.93)/g2^6 + t^5.97/g2^3 - 2*t^6. + 3*g2^3*t^6.03 + g2^6*t^6.07 + g2^12*t^6.14 + (g1^3*t^6.46)/g2^26 + (g2^22*t^6.49)/g1^3 + (g2^28*t^6.56)/g1^3 + (g1^3*t^6.6)/g2^14 + t^6.78/g2^19 + (3*t^6.89)/g2^10 + (2*t^6.92)/g2^7 + (2*t^6.95)/g2^4 + (3*t^6.99)/g2 + 3*g2^2*t^7.02 + 2*g2^5*t^7.06 + 3*g2^8*t^7.09 + 2*g2^11*t^7.13 + g2^17*t^7.19 + (g1^3*t^7.31)/g2^39 + (g2^15*t^7.41)/g1^3 + (g1^3*t^7.45)/g2^27 - (g2^18*t^7.45)/g1^3 + (g2^21*t^7.48)/g1^3 + (g2^24*t^7.52)/g1^3 - (g1^3*t^7.55)/g2^18 + (g2^27*t^7.55)/g1^3 + (g1^3*t^7.59)/g2^15 + (g1^3*t^7.62)/g2^12 + (g2^33*t^7.62)/g1^3 + (g1^3*t^7.72)/g2^3 + t^7.74/g2^23 + t^7.77/g2^20 + t^7.81/g2^17 + (3*t^7.84)/g2^14 + (2*t^7.87)/g2^11 + (3*t^7.91)/g2^8 + (4*t^7.94)/g2^5 + (4*t^7.98)/g2^2 - 2*g2*t^8.01 + 6*g2^4*t^8.05 + 2*g2^7*t^8.08 + 2*g2^10*t^8.11 + g2^13*t^8.15 + 2*g2^16*t^8.18 + g2^22*t^8.25 + (g1^3*t^8.44)/g2^28 + (g1^3*t^8.47)/g2^25 + (g2^20*t^8.47)/g1^3 + (g2^23*t^8.5)/g1^3 + (g2^26*t^8.54)/g1^3 + (g2^29*t^8.57)/g1^3 + (g1^3*t^8.58)/g2^16 + t^8.59/g2^36 + (g1^3*t^8.61)/g2^13 + t^8.66/g2^30 + t^8.69/g2^27 + t^8.73/g2^24 + t^8.76/g2^21 + (3*t^8.8)/g2^18 + (2*t^8.83)/g2^15 - t^8.86/g2^12 + (6*t^8.9)/g2^9 + (3*t^8.97)/g2^3 + t^8.97/(g2^3*y^2) - t^3.99/(g2*y) - t^4.98/(g2^2*y) - t^6./y - t^6.85/(g2^13*y) - t^6.92/(g2^7*y) - t^6.95/(g2^4*y) - (2*t^6.99)/(g2*y) - (g2^5*t^7.06)/y - t^7.84/(g2^14*y) + t^7.87/(g2^11*y) - t^7.91/(g2^8*y) + t^7.98/(g2^2*y) - (g2^4*t^8.05)/y + (g2^7*t^8.08)/y + t^8.8/(g2^18*y) + t^8.83/(g2^15*y) + (2*t^8.93)/(g2^6*y) - (t^3.99*y)/g2 - (t^4.98*y)/g2^2 - t^6.*y - (t^6.85*y)/g2^13 - (t^6.92*y)/g2^7 - (t^6.95*y)/g2^4 - (2*t^6.99*y)/g2 - g2^5*t^7.06*y - (t^7.84*y)/g2^14 + (t^7.87*y)/g2^11 - (t^7.91*y)/g2^8 + (t^7.98*y)/g2^2 - g2^4*t^8.05*y + g2^7*t^8.08*y + (t^8.8*y)/g2^18 + (t^8.83*y)/g2^15 + (2*t^8.93*y)/g2^6 + (t^8.97*y^2)/g2^3 |
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 |
---|---|---|---|---|---|---|---|---|---|
57332 | SU3adj1nf2 | ${}q_{1}^{2}\tilde{q}_{1}^{2}$ + ${ }q_{2}^{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }\phi_{1}^{2}X_{1}$ + ${ }M_{1}q_{1}\tilde{q}_{2}$ | 1.455 | 1.6425 | 0.8858 | [X:[1.3409], M:[0.9544], q:[0.5169, 0.4941], qb:[0.4831, 0.5287], phi:[0.3295]] | t^2.863 + t^2.932 + t^2.966 + t^3. + t^3.068 + t^3.92 + t^3.989 + t^4.023 + t^4.057 + t^4.126 + t^4.909 + t^4.977 + t^5.046 + t^5.114 + t^5.473 + t^5.504 + t^5.572 + t^5.61 + t^5.726 + t^5.795 + t^5.829 + t^5.863 + t^5.897 + 2*t^5.932 + t^5.966 - 2*t^6. - t^3.989/y - t^4.977/y - t^3.989*y - t^4.977*y | detail |