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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47081 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }\phi_{1}q_{1}^{2}$ + ${ }M_{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{1}^{2}$ + ${ }M_{3}\phi_{1}q_{2}\tilde{q}_{1}$ + ${ }M_{4}\phi_{1}q_{2}\tilde{q}_{2}$ + ${ }M_{2}M_{5}$ + ${ }M_{4}M_{5}$ | 0.605 | 0.7784 | 0.7772 | [X:[], M:[1.0, 0.7751, 0.6687, 0.7751, 1.2249], q:[0.7781, 0.2219], qb:[0.6657, 0.5592], phi:[0.4438]] | [X:[], M:[[0], [-8], [6], [-8], [8]], q:[[1], [-1]], qb:[[-3], [11]], phi:[[-2]]] | 1 |
Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
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${}M_{3}$, ${ }M_{4}$, ${ }q_{2}\tilde{q}_{2}$, ${ }\phi_{1}^{2}$, ${ }\phi_{1}q_{2}^{2}$, ${ }q_{2}\tilde{q}_{1}$, ${ }M_{1}$, ${ }M_{5}$, ${ }M_{3}^{2}$, ${ }q_{1}\tilde{q}_{2}$, ${ }M_{3}M_{4}$, ${ }\phi_{1}q_{1}q_{2}$, ${ }q_{1}\tilde{q}_{1}$, ${ }M_{3}q_{2}\tilde{q}_{2}$, ${ }M_{4}^{2}$, ${ }M_{3}\phi_{1}^{2}$, ${ }M_{3}\phi_{1}q_{2}^{2}$, ${ }M_{3}q_{2}\tilde{q}_{1}$, ${ }M_{4}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}\tilde{q}_{2}^{2}$, ${ }q_{2}^{2}\tilde{q}_{2}^{2}$, ${ }M_{4}\phi_{1}^{2}$, ${ }M_{4}\phi_{1}q_{2}^{2}$, ${ }M_{4}q_{2}\tilde{q}_{1}$, ${ }M_{1}M_{3}$, ${ }\phi_{1}^{2}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}q_{2}^{3}\tilde{q}_{2}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$, ${ }q_{2}^{2}\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{1}M_{4}$, ${ }\phi_{1}^{4}$, ${ }\phi_{1}^{3}q_{2}^{2}$, ${ }\phi_{1}^{2}q_{2}^{4}$, ${ }\phi_{1}^{2}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}q_{2}^{3}\tilde{q}_{1}$, ${ }\phi_{1}\tilde{q}_{1}^{2}$, ${ }q_{2}^{2}\tilde{q}_{1}^{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{2}$, ${ }M_{1}\phi_{1}^{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{1}$ | ${}$ | -3 | t^2.01 + t^2.33 + t^2.34 + 3*t^2.66 + t^3. + t^3.67 + 2*t^4.01 + 2*t^4.33 + t^4.35 + t^4.65 + 3*t^4.67 + 2*t^4.69 + 2*t^4.99 + 5*t^5.01 + 8*t^5.33 + t^5.34 + 2*t^5.66 - 3*t^6. + 3*t^6.02 - 2*t^6.32 + 4*t^6.34 + 2*t^6.36 + t^6.66 + 5*t^6.67 + 2*t^6.69 + t^6.98 + 3*t^6.99 + 4*t^7.01 + 2*t^7.03 + 2*t^7.31 + 5*t^7.33 + 7*t^7.35 + 4*t^7.65 + 8*t^7.67 + 2*t^7.69 + 13*t^7.99 - t^8.01 + 2*t^8.02 - t^8.33 - 3*t^8.34 + 4*t^8.36 - t^8.64 - 12*t^8.66 + 5*t^8.68 + 4*t^8.7 - 4*t^8.98 - t^4.33/y - t^6.34/y - t^6.66/y - t^6.99/y + t^7.33/y + t^7.35/y + (5*t^7.67)/y + (3*t^7.99)/y + (5*t^8.01)/y + (5*t^8.33)/y + (2*t^8.66)/y + t^8.68/y - t^8.98/y - t^4.33*y - t^6.34*y - t^6.66*y - t^6.99*y + t^7.33*y + t^7.35*y + 5*t^7.67*y + 3*t^7.99*y + 5*t^8.01*y + 5*t^8.33*y + 2*t^8.66*y + t^8.68*y - t^8.98*y | g1^6*t^2.01 + t^2.33/g1^8 + g1^10*t^2.34 + (3*t^2.66)/g1^4 + t^3. + g1^8*t^3.67 + 2*g1^12*t^4.01 + (2*t^4.33)/g1^2 + g1^16*t^4.35 + t^4.65/g1^16 + 3*g1^2*t^4.67 + 2*g1^20*t^4.69 + (2*t^4.99)/g1^12 + 5*g1^6*t^5.01 + (8*t^5.33)/g1^8 + g1^10*t^5.34 + (2*t^5.66)/g1^4 - 3*t^6. + 3*g1^18*t^6.02 - (2*t^6.32)/g1^14 + 4*g1^4*t^6.34 + 2*g1^22*t^6.36 + t^6.66/g1^10 + 5*g1^8*t^6.67 + 2*g1^26*t^6.69 + t^6.98/g1^24 + (3*t^6.99)/g1^6 + 4*g1^12*t^7.01 + 2*g1^30*t^7.03 + (2*t^7.31)/g1^20 + (5*t^7.33)/g1^2 + 7*g1^16*t^7.35 + (4*t^7.65)/g1^16 + 8*g1^2*t^7.67 + 2*g1^20*t^7.69 + (13*t^7.99)/g1^12 - g1^6*t^8.01 + 2*g1^24*t^8.02 - t^8.33/g1^8 - 3*g1^10*t^8.34 + 4*g1^28*t^8.36 - t^8.64/g1^22 - (12*t^8.66)/g1^4 + 5*g1^14*t^8.68 + 4*g1^32*t^8.7 - (4*t^8.98)/g1^18 - t^4.33/(g1^2*y) - (g1^4*t^6.34)/y - t^6.66/(g1^10*y) - t^6.99/(g1^6*y) + t^7.33/(g1^2*y) + (g1^16*t^7.35)/y + (5*g1^2*t^7.67)/y + (3*t^7.99)/(g1^12*y) + (5*g1^6*t^8.01)/y + (5*t^8.33)/(g1^8*y) + (2*t^8.66)/(g1^4*y) + (g1^14*t^8.68)/y - t^8.98/(g1^18*y) - (t^4.33*y)/g1^2 - g1^4*t^6.34*y - (t^6.66*y)/g1^10 - (t^6.99*y)/g1^6 + (t^7.33*y)/g1^2 + g1^16*t^7.35*y + 5*g1^2*t^7.67*y + (3*t^7.99*y)/g1^12 + 5*g1^6*t^8.01*y + (5*t^8.33*y)/g1^8 + (2*t^8.66*y)/g1^4 + g1^14*t^8.68*y - (t^8.98*y)/g1^18 |
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 |
---|---|---|---|---|---|---|---|---|---|
46535 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }\phi_{1}q_{1}^{2}$ + ${ }M_{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{1}^{2}$ + ${ }M_{3}\phi_{1}q_{2}\tilde{q}_{1}$ + ${ }M_{4}\phi_{1}q_{2}\tilde{q}_{2}$ + ${ }M_{2}M_{5}$ | 0.6253 | 0.8097 | 0.7722 | [X:[], M:[1.0, 0.9511, 0.7439, 0.7439, 1.0489], q:[0.7561, 0.2439], qb:[0.5244, 0.5244], phi:[0.4878]] | 2*t^2.23 + 2*t^2.3 + 2*t^2.93 + t^3. + t^3.15 + 2*t^3.84 + 3*t^4.46 + 4*t^4.54 + 6*t^4.61 + 2*t^5.16 + 6*t^5.23 + 2*t^5.3 + 2*t^5.38 + 2*t^5.45 + 3*t^5.85 + t^5.93 - 5*t^6. - t^4.46/y - t^4.46*y | detail |