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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60034 | SU3adj1nf2 | ${}q_{1}q_{2}\tilde{q}_{1}^{2}$ + ${ }M_{1}\phi_{1}q_{1}\tilde{q}_{2}$ + ${ }M_{1}^{2}$ + ${ }q_{1}\tilde{q}_{2}X_{1}$ + ${ }M_{2}\phi_{1}q_{1}\tilde{q}_{1}$ | 1.3614 | 1.5889 | 0.8568 | [X:[1.376], M:[1.0, 0.744], q:[0.3151, 0.5551], qb:[0.5649, 0.3089], phi:[0.376]] | [X:[[0, 1]], M:[[0, 0], [0, -6]], q:[[-1, -1], [-1, -11]], qb:[[1, 6], [1, 0]], phi:[[0, 1]]] | 2 |
Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
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${}M_{2}$, ${ }\phi_{1}^{2}$, ${ }q_{2}\tilde{q}_{2}$, ${ }q_{1}\tilde{q}_{1}$, ${ }M_{1}$, ${ }q_{2}\tilde{q}_{1}$, ${ }\phi_{1}^{3}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}^{2}q_{1}\tilde{q}_{2}$, ${ }X_{1}$, ${ }M_{2}^{2}$, ${ }M_{2}\phi_{1}^{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}^{4}$, ${ }\phi_{1}q_{1}^{2}q_{2}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}^{2}$, ${ }M_{2}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}^{2}q_{2}\tilde{q}_{2}$, ${ }M_{2}q_{1}\tilde{q}_{1}$, ${ }\phi_{1}^{2}q_{1}\tilde{q}_{1}$, ${ }q_{2}^{2}\tilde{q}_{2}^{2}$, ${ }M_{1}M_{2}$, ${ }M_{1}\phi_{1}^{2}$, ${ }\phi_{1}q_{1}q_{2}^{2}$, ${ }\phi_{1}\tilde{q}_{1}^{2}\tilde{q}_{2}$, ${ }M_{2}q_{2}\tilde{q}_{1}$, ${ }M_{1}q_{2}\tilde{q}_{2}$, ${ }M_{2}\phi_{1}^{3}$, ${ }\phi_{1}^{2}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}^{5}$, ${ }M_{1}q_{1}\tilde{q}_{1}$, ${ }\phi_{1}^{2}\tilde{q}_{1}\tilde{q}_{2}^{2}$, ${ }\phi_{1}^{2}q_{1}^{2}q_{2}$, ${ }M_{2}\phi_{1}q_{2}\tilde{q}_{2}$, ${ }q_{2}^{2}\tilde{q}_{1}\tilde{q}_{2}$, ${ }\phi_{1}^{3}q_{2}\tilde{q}_{2}$ | ${}$ | -2 | t^2.23 + t^2.26 + t^2.59 + t^2.64 + t^3. + t^3.36 + t^3.38 + t^3.72 + 2*t^4.13 + t^4.46 + 2*t^4.49 + t^4.51 + 2*t^4.68 + t^4.82 + 2*t^4.85 + t^4.87 + 2*t^4.9 + t^5.18 + t^5.23 + t^5.26 + t^5.4 + t^5.44 + 2*t^5.59 + 3*t^5.62 + 2*t^5.64 + t^5.8 + t^5.81 + 2*t^5.95 + 2*t^5.98 - 2*t^6. + t^6.02 + t^6.16 + t^6.22 + t^6.31 + 3*t^6.36 + 3*t^6.38 - t^6.41 + t^6.53 + t^6.57 + t^6.7 + 5*t^6.72 + 2*t^6.74 + 3*t^6.77 + t^6.91 + 2*t^6.93 + 2*t^6.94 - t^6.96 + t^7.06 + 4*t^7.08 + 4*t^7.1 + 2*t^7.13 + 2*t^7.15 + t^7.27 + t^7.28 + t^7.42 + 3*t^7.44 + 4*t^7.49 + 2*t^7.51 + t^7.64 + 2*t^7.66 + t^7.68 + 2*t^7.7 + t^7.78 + 2*t^7.82 + 7*t^7.85 + 3*t^7.87 + 2*t^7.9 + t^8. + 3*t^8.04 + 2*t^8.06 + 2*t^8.07 - t^8.08 - t^8.09 + 3*t^8.18 + 6*t^8.21 + 2*t^8.26 + 2*t^8.28 + t^8.38 + 5*t^8.4 - t^8.43 + t^8.45 + t^8.47 + t^8.48 + 2*t^8.54 + 3*t^8.57 - t^8.59 + 7*t^8.62 - t^8.64 - t^8.66 + 2*t^8.76 - t^8.78 + 2*t^8.79 + 3*t^8.8 + t^8.81 + 2*t^8.83 - t^8.84 - t^8.85 + t^8.86 + t^8.9 + t^8.93 + 5*t^8.95 + 9*t^8.98 - t^4.13/y - t^5.26/y - t^6.36/y - t^6.38/y - t^6.72/y - t^6.77/y - t^7.49/y - (2*t^7.51)/y + t^7.82/y + (2*t^7.87)/y + t^7.9/y + (2*t^8.23)/y - t^8.26/y + t^8.59/y + t^8.95/y - t^4.13*y - t^5.26*y - t^6.36*y - t^6.38*y - t^6.72*y - t^6.77*y - t^7.49*y - 2*t^7.51*y + t^7.82*y + 2*t^7.87*y + t^7.9*y + 2*t^8.23*y - t^8.26*y + t^8.59*y + t^8.95*y | t^2.23/g2^6 + g2^2*t^2.26 + t^2.59/g2^11 + g2^5*t^2.64 + t^3. + t^3.36/g2^5 + g2^3*t^3.38 + t^3.72/g2^10 + 2*g2*t^4.13 + t^4.46/g2^12 + (2*t^4.49)/g2^4 + g2^4*t^4.51 + t^4.68/(g1^3*g2^12) + g1^3*g2^7*t^4.68 + t^4.82/g2^17 + (2*t^4.85)/g2^9 + t^4.87/g2 + 2*g2^7*t^4.9 + t^5.18/g2^22 + t^5.23/g2^6 + g2^2*t^5.26 + t^5.4/(g1^3*g2^22) + g1^3*g2^13*t^5.44 + (2*t^5.59)/g2^11 + (3*t^5.62)/g2^3 + 2*g2^5*t^5.64 + g1^3*g2^8*t^5.8 + t^5.81/(g1^3*g2^11) + (2*t^5.95)/g2^16 + (2*t^5.98)/g2^8 - 2*t^6. + g2^8*t^6.02 + g1^3*g2^3*t^6.16 + t^6.22/g1^3 + t^6.31/g2^21 + (3*t^6.36)/g2^5 + 3*g2^3*t^6.38 - g2^11*t^6.41 + t^6.53/(g1^3*g2^21) + g1^3*g2^14*t^6.57 + t^6.7/g2^18 + (5*t^6.72)/g2^10 + (2*t^6.74)/g2^2 + 3*g2^6*t^6.77 + g1^3*g2*t^6.91 + 2*g1^3*g2^9*t^6.93 + (2*t^6.94)/(g1^3*g2^10) - g1^3*g2^17*t^6.96 + t^7.06/g2^23 + (4*t^7.08)/g2^15 + (4*t^7.1)/g2^7 + 2*g2*t^7.13 + 2*g2^9*t^7.15 + (g1^3*t^7.27)/g2^4 + t^7.28/(g1^3*g2^23) + t^7.42/g2^28 + (3*t^7.44)/g2^20 + (4*t^7.49)/g2^4 + 2*g2^4*t^7.51 + t^7.64/(g1^3*g2^28) + (2*t^7.66)/(g1^3*g2^20) + g1^3*g2^7*t^7.68 + 2*g1^3*g2^15*t^7.7 + t^7.78/g2^33 + (2*t^7.82)/g2^17 + (7*t^7.85)/g2^9 + (3*t^7.87)/g2 + 2*g2^7*t^7.9 + t^8./(g1^3*g2^33) + t^8.04/(g1^3*g2^17) + 2*g1^3*g2^2*t^8.04 + 2*g1^3*g2^10*t^8.06 + (2*t^8.07)/(g1^3*g2^9) - g1^3*g2^18*t^8.08 - t^8.09/(g1^3*g2) + (3*t^8.18)/g2^22 + (6*t^8.21)/g2^14 + 2*g2^2*t^8.26 + 2*g2^10*t^8.28 + t^8.38/(g1^3*g2^30) + (2*t^8.4)/(g1^3*g2^22) + (3*g1^3*t^8.4)/g2^3 - t^8.43/(g1^3*g2^14) + t^8.45/(g1^3*g2^6) + g1^3*g2^21*t^8.47 + (g2^2*t^8.48)/g1^3 + (2*t^8.54)/g2^27 + (3*t^8.57)/g2^19 - t^8.59/g2^11 + (7*t^8.62)/g2^3 - g2^5*t^8.64 - g2^13*t^8.66 + t^8.76/(g1^3*g2^27) + (g1^3*t^8.76)/g2^8 - g1^3*t^8.78 + (2*t^8.79)/(g1^3*g2^19) + 3*g1^3*g2^8*t^8.8 + t^8.81/(g1^3*g2^11) + 2*g1^3*g2^16*t^8.83 - t^8.84/(g1^3*g2^3) - g1^3*g2^24*t^8.85 + (g2^5*t^8.86)/g1^3 + t^8.9/g2^32 + t^8.93/g2^24 + (5*t^8.95)/g2^16 + (9*t^8.98)/g2^8 - (g2*t^4.13)/y - (g2^2*t^5.26)/y - t^6.36/(g2^5*y) - (g2^3*t^6.38)/y - t^6.72/(g2^10*y) - (g2^6*t^6.77)/y - t^7.49/(g2^4*y) - (2*g2^4*t^7.51)/y + t^7.82/(g2^17*y) + (2*t^7.87)/(g2*y) + (g2^7*t^7.9)/y + (2*t^8.23)/(g2^6*y) - (g2^2*t^8.26)/y + t^8.59/(g2^11*y) + t^8.95/(g2^16*y) - g2*t^4.13*y - g2^2*t^5.26*y - (t^6.36*y)/g2^5 - g2^3*t^6.38*y - (t^6.72*y)/g2^10 - g2^6*t^6.77*y - (t^7.49*y)/g2^4 - 2*g2^4*t^7.51*y + (t^7.82*y)/g2^17 + (2*t^7.87*y)/g2 + g2^7*t^7.9*y + (2*t^8.23*y)/g2^6 - g2^2*t^8.26*y + (t^8.59*y)/g2^11 + (t^8.95*y)/g2^16 |
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 |
---|---|---|---|---|---|---|---|---|---|
57729 | SU3adj1nf2 | ${}q_{1}q_{2}\tilde{q}_{1}^{2}$ + ${ }M_{1}\phi_{1}q_{1}\tilde{q}_{2}$ + ${ }M_{1}^{2}$ + ${ }q_{1}\tilde{q}_{2}X_{1}$ | 1.3423 | 1.5531 | 0.8642 | [X:[1.3749], M:[1.0], q:[0.3123, 0.5632], qb:[0.5623, 0.3128], phi:[0.3749]] | t^2.25 + t^2.62 + t^2.63 + t^3. + t^3.37 + t^3.38 + 2*t^3.75 + 2*t^4.12 + 2*t^4.5 + 2*t^4.69 + 2*t^4.87 + 2*t^4.88 + t^5.25 + t^5.26 + 2*t^5.44 + 2*t^5.62 + 3*t^5.63 + 2*t^5.81 + 3*t^6. - t^4.12/y - t^5.25/y - t^4.12*y - t^5.25*y | detail |